PY 120 Laboratory Manual
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Wayne Warrick Passaic County Community College Laboratory Manual PY-120 Physics I
Laboratory Manual PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction As part of the Passaic County Community College physics course sequence, the laboratory is a required and integral component to all offered physics courses within the Biological and Physical Sciences Department. This manual will act as a comprehensive reference guide for students to follow during each laboratory experiment. The following pages will detail the laboratory grading criteria, expected report format, laboratory safety and etiquette protocol, and detailed instructions for each experiment. Each laboratory section of this manual includes the necessary theoretical background, pertaining to physics, in order for students to perform each experiment. The laboratory aspect of physics, as with any physical or life science course, represents a necessary part to gather not only an adequate understanding of physics but to obtain a solid foundation which will benefit students of all STEM majors. This is why it is highly recommended to read through this manual, ahead of time, so that you are prepared to not only follow along in the lab, but to actively engage with each of your colleagues and understand each experiment. Additional references, links, and helpful websites are listed within each experiment section. Copyright: Wayne Warrick, 2022 Laboratory Manual Authored by Wayne Warrick May 2019 Rev: July 2023
Table of Contents Laboratory Requirements
___________________________________________________________ 1
Lab Report Grading Criteria
________________________________________________________ 2 Laboratory Report Format
__________________________________________________________ 3 Laboratory 1: Data Acquisition and Data Analysis________________________________________ 4 Laboratory 1: Prelab_______________________________________________________________ 11 Laboratory 2: Free-Fall_____________________________________________________________15 Laboratory 2: Prelab_______________________________________________________________ 16 Laboratory 3: Projectile Motion______________________________________________________18 Laboratory 3: Prelab_______________________________________________________________20 Laboratory 4: Newton’s Second Law of Motion_________________________________________ 23 Laboratory 4: Prelab_______________________________________________________________24 Laboratory 5: Friction Analysis ______________________________________________________27
Laboratory 5: Prelab_______________________________________________________________ 30
Laboratory 6: The Conservation of Mechanical Energy____________________________________ 33 Laboratory 6: Prelab_______________________________________________________________ 34
Laboratory 7: The Conservation of Linear Momentum____________________________________ 36
Laboratory 7: Prelab_______________________________________________________________ 37
Laboratory 8: The Ballistic Pendulum_________________________________________________ 41
Laboratory 8:
Prelab_______________________________________________________________ 42
Laboratory 9: Uniform Circular Motion________________________________________________ 44
Laboratory 9: Prelab_______________________________________________________________ 45
Laboratory 10: Rotational Dynamics__________________________________________________ 48
Laboratory 10: Prelab______________________________________________________________50
Laboratory 11: Conservation of Angular Momentum _____________________________________52 Laboratory 12:
Fluid Dynamics and Heat Exchange_______________________________________55 References
______________________________________________________________________ 57
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1 Laboratory Requirements PY-120 Physics I Laboratory Passaic County Community College Professor: Wayne Warrick The laboratory portion of the course counts towards 25% of the final course grade. Unless otherwise stated, each experiment will require a written report. Each lab report will be graded out of a total of 10 points. The required format for lab reports is detailed in the Laboratory Report Format section of this manual and a Sample Report is provided on Blackboard. Laboratory assessment is divided into the following categories: Prelab, Participation, Experimental Data Collection, and the submitted Lab Report. Each of these categories and grading criteria is explained below. Prelab The prelab is intended to prepare students for the laboratory experiment. Before handling sensitive apparatus, equipment, or computer-controlled data collection tools, etc., it is necessary to have an adequate understanding of the experiment. The prelab will test your knowledge and comprehension of the physics required to perform the experiment and demonstrate each student’s level of procedural preparedness. The prelab for each experiment can be found in the lab manual. Do not print these pages out. Read the lab manual in preparation for the week’s upcoming experiment and be able to correctly answer at least three out of five of the prelab questions. All of the answers to the prelab questions can be found in the lab manual. When you arrive to the lab the instructor will hand out the prelabs. You will have 15 minutes to complete and submit. The prelabs will be graded as soon as they are handed in. Students who do not pass the prelab are not permitted to perform the experiment for that week and will receive a grade of zero for the lab report.
Read Ahead!
It is imperative to read the lab manual and lab procedures prior to performing each experiment. Participation Laboratory attendance is mandatory. Students are expected to answer the prelab questions, participate in the experiment, collect data, and answer questions posed by the instructor. Additional details regarding the attendance portion of the lab can be found on the course syllabus. Lab Safety The instructor will discuss the safety aspects of each experiment at the beginning of the laboratory. Experimental Data
During each lab experiment, students will collect data, often a lot of data. Sometimes this is manual data, read from protractors, meter sticks, and scales, other times it is data from electronic instrumentation. It is required that each student record their data from each experiment in a lab notebook. Report Lab reports are required for each experiment. Each group will submit one lab report corresponding to each lab. All parts of the lab report must be typed up. The only exceptions are sketches and calculations, which can be hand-written. If there are multiple trials, it is only necessary to show calculations for one trial. The format for the report can be found in the Laboratory Report Format section of this lab manual. A sample lab report can be found on Blackboard. The lab report must adhere to this format.
2 Lab Report Grading Criteria Each lab report is graded out of 10 points. The grading is based on the following criteria: •
Was the report submitted by the due date? Refer to the syllabus. •
Does the report adhere to the Laboratory Report Format? •
Does the report include the abstract? •
Does the abstract include a brief summary of the critical results, values and findings from the experiment? Critical results are numerical values that you consider to be the most critical. •
Does the lab report contain and present all of the required experimental data? •
Does the report contain applicable data tables? •
Does the lab report contain data analysis and all of the required calculations? •
Does the report contain all of required plots, with title, axes labeled and units? •
Were all of the questions answered correctly and in complete sentences? •
Does the lab report contain plagiarized content? If points are deducted from a report, feedback will be provided on Blackboard. Please review this feedback to make corrections to future lab reports. Careful!
If a lab report contains data, pictures, answers, etc. obtained from external sources, for example, the Internet, other lab groups, etc., this will count as plagiarism, and the group will receive a zero for that report. Lab Report Submission The completed lab reports must be submitted electronically as one file.
The report should be a Microsoft Word document so that Blackboard SafeAssign can easily read it. All PCCC students have free access to Microsoft Office which includes Word and Excel. The group must decide who will be responsible for submitting the report. The completed lab report must be submitted through Blackboard SafeAssign. Emailed reports will not be accepted. The due date for each report can be found on the course syllabus. If the lab report is not submitted on time, 25% will be deducted every day after the due date. Reports submitted a fraction of a full day late will receive a proportional fraction of the deduction. Late reports must also be submitted through Blackboard SafeAssign. If a student is repeating the course, they are not permitted to submit the same lab report from a previous semester. Lab Final Exam There will be a cumulative lab final exam at the end of the semester based on the experiments performed in the lab. The lab final exam will count towards 20% of the lab portion of the course. Prepare for this exam be reviewing previous experiments as found in the lab manual. As a reminder, if a student fails the lab portion of the course, the student will receive a failing grade (F) for the course. Please review the course syllabus for additional details regarding the laboratory policies.
3 Laboratory Report Format PY-120 Physics I Laboratory Passaic County Community College Professor: Wayne Warrick Begin the lab report with the following information. Lab # Lab Title Lab Group Members: First and Last Name of each student Date of Experiment:
mm/dd/year Professor’s Name: Abstract An abstract is a brief overall summary of the experiment. The abstract should be written as though you were explaining this to a colleague as a summary of the experiment. A reader should be able to grasp a basic understanding of what happened during the experiment simply by reading the abstract. It is preferred to use the active voice. This means that you write as though the event was recently performed in the lab, not in the past. For example: instead of writing “we studied,” you should write “in this experiment we study the effects of...” Here, you will also summarize the conclusions from the experiment. The abstract only needs to be one paragraph. Include a brief summary of the critical results, numerical values and findings in the abstract. Results and Analysis In this section, you will present your experimental results. This is where you report your data, equations, calculations, tables, graphs, etc. Be sure to show all pertinent calculations. Number the tables, graphs, pictures, etc. Label each axis of a graph and include units. Do not copy material from the instructor’s lab manual. Briefly discuss the results of the experiment and include discrepancies between measured and experimental results. Questions In the lab report, include the complete answers to all questions in the lab manual pertaining to the specific experiment. A Sample Lab Report is available in Blackboard.
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4 Laboratory 1 Data Acquisition and Data Analysis
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The objective of this laboratory is to introduce students to data acquisition and data analysis techniques used in physics. Students will acquire data by performing a simple kinematic experiment. By the end of the lab, students should be able to analyze data, perform calculations involving experimental error, determine the standard deviation, calculate error propagation, and perform graphical analysis. 1. Experimental Error All measurements have some type of error. An error is not a "mistake," rather it is an inherent part of the measurement process. Measurement error is the difference between the measured or observed value (quantity) and its “true” value. By “true” value, we mean a recognized standard or agreed upon accepted value. Accuracy
of a measurement is how close the measured value is to the standard value of the quantity being measured. Therefore, errors reduce the accuracy of a measurement. There are two main categories of measurement errors: random errors and systematic errors. Random errors
, as the name suggests, are unpredictable during the experiment. They are caused by unknown or unpredictable occurrences in an experiment, e.g., temperature variations, electrical noise, mechanical vibrations, etc. When a measurement is repeated, the next value is unpredictable due to fluctuations in readings of the apparatus or in your interpretation of the instrument. We cannot usually control random errors. All of the statistical methods discussed here only hold for random errors. Regardless of the type of instrument you use to make a measurement, you need to either calibrate, or verify the instrument is calibrated. When the instrument is not calibrated correctly, systematic error will result where the measured values are consistently inconsistent with the standard values. If you can identify the error, it might be possible to eliminate it. Zero error
is a type of systematic error which occurs when the instrument does not read zero when it should. Think of a bathroom scale that is not correctly calibrated and reads 5 lb. at the zero mark. Each measurement will be consistently offset by +5 lb. For example, if your “true” weight is 135 lb., the offset scale will read 140 lb. Errors that occur in an experiment that are not random or systematic can be classified as personal errors and can include mistakes made by the experimenter. While looking at an analog scale, viewed from the wrong angle, your eyes will distort the reading, due to what is called parallax error
. For example, when you look down at your car gas gauge, the pointer looks like it is on the E, but when you place your head back a little, and observe the gauge straight on, the pointer is slightly above the E mark. In the case of a ruler, tape measure, or any apparatus which has gradations, the smallest gradation is called the least count. The reading error
is one-half of the least count. For a standard ruler the least count is 1.0 mm. The reading error is, ±
0.5 mm. If you measure the length of a tube as 9.36 cm, you would report this as 9.36 ±
0.05 cm. Notice that the error has the same number of decimal places as the measurement. If you require high precision a Vernier caliper or micrometer should be used instead. The precision
of a measurement is a measure of how reproducible experimental values are, i.e., how close a number of measurements of the same quantity agrees with each other. The deviation of data is called the range. The smaller the range, the more precise the result. The precision is also limited by random errors and instrument limitations. This can usually be reduced by repeating the measurements.
5 From Figure 1, try to determine which target (bull’s-eye) represents accuracy and precision. Figure 1.
Bull’s-eye target with black dots representing trials. Images: [1]. 2. Analysis of One or Two Measurements If you want to compare a measured value to the standard value, you need to calculate the percent error. % Error =
Experimental Value − Standard Value
Standard Value
x 100%
If the standard value is a theoretical value, i.e., obtained from theoretical calculations, the percent error can be written as, % Error =
Experimental Value − Theoretical Value
Theoretical Value
x 100%
If you want to compare two measured values to each other, you need to calculate the percent difference. % Difference = <
Exp. Value 1 − Exp. Value 2
Average of these two values
< x 100%
Example The measured value of the acceleration due to gravity is 9.65 m/s
2
. The standard value is 9.81 m/s
2
. The % Error is -1.63 %. The minus sign indicates that the measured value is below the standard value. The % Difference is 1.64 %. The % Error and the % Difference are written with two decimal places. As a rule, the % Error and % Difference cannot have more decimal places than your measured values. 3. How to Present Data in a Report All measured values must be reported with their error. The word error is interchangeable with uncertainty. For example, you measured the mass of an object to be 10.923 g, but you were only confident of this value to within a measurement uncertainty of 0.2 g. In other words, the mass could be as high as 10.923 + 0.2 g or as low as 10.923 – 0.2 g. Notice how the 9 is the “doubtful” figure. So, if the 9 is doubtful, then for certain, the numbers that come after are even more uncertain, and can be ignored. The proper way to report this measurement is to write Mass = 10.9 ±
0.2 g. With high probability, the mass is within the range 10.7 g to 11.1 g. The uncertainty, 0.2 g, has one significant figure. In general, measurement uncertainty can only have one significant figure. Also, it is necessary to round the measured value to the same number of decimal places as the uncertainty. Make sure you are consistent when reporting uncertainty.
6 Example The speed of an object is measured to be: 0.32812 m/s with an uncertainty of 0.05 m/s. The uncertainty has one significant figure and two decimal places. This should be reported as: 0.33 ±
0.05 m/s. Analog vs. Digital Meters For analog scales, report your uncertainty as the reading error. For digital scales, report the uncertainty as one-half of the last digit. For example, if a digital thermometer has a precision of 1/10 of K, i.e., 0.1 K. The reported uncertainty would then be 0.05 K. If you measure the temperature of a sample as 25.80 K, you would report this 25.80 ±
0.05 K. 4. Absolute and Fractional Error Absolute error is the difference between the mean value and the i
th measured value. This can be expressed as, ∆࠵?
!
= ࠵?̅ − ࠵?
!
∆࠵?
"
= ࠵?̅ − ࠵?
"
, ∆࠵?
#
= ࠵?̅ − ࠵?
#
+,...
∆࠵?
$
= ࠵?̅ − ࠵?
$
. N is the number of measurements. The mean value of the absolute errors is, ∆࠵?
((((
$
=
∑
∆࠵?
!
$
! & "
࠵?
Fractional error is the ratio of the absolute error to the measured value. The fractional error for one measurement is ∆(
(
. The fractional error for N measurements is, ∆(
))))
(̅
. 5. Error Propagation Imagine an experiment that consists of measuring two values. One value is the distance. The other value is time. You want to calculate the speed and report its error. Both the distance and the time have error. How do you take the errors of the distance and time into account when calculating the speed? The process that we need to use is called error propagation. In other words, we need to consider the error of each measurement in order to calculate the error of the final result. A general formula we can use to determine the error of any function F(x, y, z) is, ∆࠵? =
,
-
࠵?࠵?
࠵?࠵?
∆࠵?/
#
+ -
࠵?࠵?
࠵?࠵?
∆࠵?/
#
+ -
࠵?࠵?
࠵?࠵?
∆࠵?/
#
This equation involves partial differentiation which is out of the scope of this course. Fortunately, for this course, we do not have to use this formula. We can use some shortcuts and approximations.
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7 Adding or Subtracting Error Consider a function F, which is dependent on two variables a and b. We write this as F(a, b). a and b both have their own uncertainty. How can we determine the uncertainty of F(a, b)? It will help to see this through an example. F(a, b) = a + b. This means that the function adds a and b together. ࠵? = 2.5 ± 0.7࠵?/࠵?
#
࠵? = 2.8 ± 0.2࠵?/࠵?
#
When we add a and b, we get 5.3. We do not want to simply add the absolute errors together, rather we need to use the following formula. ∆࠵? = >(∆࠵?)
#
+ (∆࠵?)
#
∆࠵?
is the error associated with the function F. ∆࠵?
and ∆࠵?
are the absolute errors associated with a and b respectively. In this example, ∆࠵?
= 0.7 and ∆࠵?
= 0.2. Using the above equation, ∆࠵?
= 0.73 m/s
2
. The correct way to report this is, F = 5.3 ±
0.7 m/s
2
. As a general rule, if the uncertainty of one measurement is at least three times greater than the error of another measurement, the larger error dominates. It you are measuring the same type of quantity using the same instrument, the error should be the same for each trial. Example:
L
1
= 2.50 ±
0.05 cm and L
2
= 5.00 ±
0.05 cm. Determine the sum of these lengths. F = L
1
+ L
2
= 7.50 ±
0.07 cm Even when subtracting values, we still add the uncertainties since overall uncertainty increases (it is compounded). Example:
During a filtration experiment 4.22 ±
0.03g remains on the filter paper. The initial amount was 5.23 ±
0.03g. How much quantity was sifted from the paper? 5.23 g – 4.22 g = 1.01 ±
0.04 g Multiplying or Dividing Error Consider a function F, which is dependent on two variables v and t. We write this as F(v, t). v and t both have their own uncertainty. How can we determine the uncertainty of F(v, t)? It will help to see this through an example. F(v, t) = v ×
t. This means that the function takes the product of v and t. v = 15.35 ± 0.1 ࠵?/࠵?
t = 8.2567 ± 0.03 ࠵?
To determine the uncertainty associated with the function F, we need to use the equation. ∆࠵? = ࠵? ×
,
-
∆࠵?
࠵?
/
#
+ -
∆࠵?
࠵?
/
#
8 First, round each measurement so that it has the same number of decimals as the error. ∆࠵?
is the error associated with the function F. ∆࠵?
is the error in v. ∆࠵?
is the error in t. The uncertainties under the radical are fractional or relative errors. From this example, ∆࠵? = 0.95
. It may be tempting to write the final answer as F = v ×
t = 127.2 ± 0.95 m
. However, the error can only have one significant figure. Round the error 0.95 to 1. The error has no decimal places (refer to page 5). The final value is F = 127 ±
1 m. Example
: mass = 25.0 ±
0.5 g, volume = 10.0 ±
0.1 cm
3
. Calculate the density and the percent uncertainty of the density. ࠵?
= mass/volume = 2.5. The fractional error of the density is, ∆࠵? = ࠵? ×
,
-
∆࠵?
࠵?
/
#
+ -
∆࠵?
࠵?
/
#
∆࠵?
= 0.06 cm
3
. This can be rounded to 0.1 cm
3
. Report the density as ࠵?
= 2.5 ±
0.1 cm
3
Example You measure the following linear dimensions: L = 2.0 ±
0.1 m, W = 3.5 ±
0.1 m, H = 4.0 ±
0.2 m You may be tempted to write the volume as V = 28.0 ±
2.1 m
3
. The uncertainty needs to be rounded to 2 m
3
. The final value is, V = 28 ±
2 m
3
. If you have a function of the form, F = a
m
b
n
, then you can find the error of F using the following equation. ∆F = F ×
,
m -
∆a
a
/
#
+ n -
∆b
b
/
#
If you have a function of the form, F = +
!
,
"
-
#
, then you can find the error of F using the following approximation, ∆F = F × -m
∆a
a
+ q
∆b
b
+ p
∆c
c
/
How to Report Error This is really a preference of the person collecting the data. A common format is: 2.50 g/cm
3
±
3.0% The unit is placed after the measured value. The 3% is the percent error. 2.50 ±
0.07 g/cm
3
. The unit is placed after the absolute error. 0.07 is the absolute error and is 3% of the measured value. 6. Data Analysis A good experiment requires repetition, called trials. For every trial, one or more measurements are made. For every measurement, there is some inherent error. In physics, we want to perform at least three trails. All of the measured numerical values you obtain during each trial is called data. What type of data analysis you perform depends on what the experiment requires. A very common statistical quantity is the mean or average of the data. A review on how to calculate the mean can be found in the Physics Preparation Guide. Another, even more important statistical quantity is called the standard deviation.
9 7. Standard Deviation Standard deviation is numerical value that indicates how much the data is spread out when random errors are present. It tells us how much the data varies from the mean. The figure below illustrates a histogram. A “best-fit” bell curve (Gaussian or Normal distribution), which illustrates the range or spread of the measurements, has been placed over the histogram. The mean of the measured quantities is on the x-axis located at the center of the curve. Consider student’s exam scores ranging from 0 to 100. Let the x-axis be segments of the score range 100-91, 90-81, etc. Let the y-axis be the frequency (height) of those scores. The number of students receiving a grade between 91-100 would be the frequency for that grade range. The histogram would have a bin width of 10 (i.e., all possible scores between 91 and 100). The greater the number of students receiving a particular score, the taller the bar and closer to the center. The width (sharpness) of the curve is characterized by the standard deviation. From here on we will use the symbol s
to represent the standard deviation. 1
࠵?
tells us that 68% of the data is centered around the mean. 2
s
indicates that 95% of the data is centered around the mean. 3
s
indicates that 99.7% of the data is centered around the mean. A low s
tells us that the data is close (clustered) around the mean and indicates high precision. A high s
tells us that the data is spread out far from the mean. Figure 2. Histogram plot of the data with a "best-fit" curve [2].
How to Calculate the Standard Deviation: 1)
Calculate the mean of the data, which is called
࠵?
(
. 2)
The variance can be expressed as, ࠵?
#
=
"
$."
∑
(࠵? − ࠵?
(
)
#
$
!&"
. N is the number of measurements or trials. X is an individual value. 3)
The SD is the square root of the variance and can be written as, ࠵? = U
"
$."
∑
(࠵? − ࠵?
(
)
#
$
!&"
. It is highly recommended to calculate the standard deviation using software. Use the function STDEV in Excel. Once you know your standard deviation, you can report your results. They should take the form, ࠵?̅ ± ࠵?
indicates 68% of measured values are centered around one standard deviation. ࠵?̅ ± 2࠵?
indicates 95% of measured values are centered around two standard deviations. ࠵?̅ ± 3࠵?
indicates 99.7% of measured values are centered around three standard deviations. Best-fit curve
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10 Example The acceleration due to gravity (g) is measured five times in an experiment. The reported values are: 9.62, 9.65, 9.71, 9.73, 9.80 with units of m/s
2
. The average value of g is 9.70 m/s
2
. The standard value of g is 9.80 m/s
2
. The standard deviation of g is 0.07 m/s
2
. This means that values of g within the range of 9.70 ±
0.07 m/s
2
have a 68% chance of being found. Notice that the standard deviation is the uncertainty. As required, the uncertainty has one significant figure and two decimal places. The measured value of g has two decimal places. Values of g within the range 9.70 ±
2
s
have a 95% chance of being found. You cannot report this as 9.70 ±
0.14 m/s
2
because the uncertainty has two significant figures. Round the uncertainty to 0.1. Now, the uncertainty has one decimal place. Round the measured value to 9.7. The correct way to report the values of g within 2
s
is 9.7 ±
0.1 m/s
2
. If you have multiple trials, and each trial contains a quantity that results from error propagation, you can use the following technique. Trial 1: S
1
= Value ±
Error Trial 2: S
2
= Value ±
Error ... Trial N: S
N
= Value ±
Error. The error for each trial results after using error propagation. The average value of S is simple the mean of all of the trials. The error of the average value is ∆S
(
= (S
/01
+ Error of ࠵?
2+(
) − (S
/34
− Error of ࠵?
2!5
)
S
max
is the largest value of S. S
min
is the smallest value of S. 8. Data Outliers If a data point lies beyond or outside of what was consistent with the data trend, do not ignore this. Take a close look to determine what may have caused the outlier. A test that you can use to determine if the data point is truly an outlier is to compare it to 3
࠵?
. If the data point is less than 3
࠵?
, keep it. If the data point is greater than 3
࠵?
you can exclude that data point. Be sure to discuss this as a discrepancy in the lab report.
11 Laboratory 1-Prelab Data Acquisition and Data Analysis
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 List two types of specific measurement errors you expect to encounter in this lab. Question 2 If the gradations of the meter stick are one millimeter, how will you determine the reading error of the meter stick? Question 3 Write down the expressions for percent error and percent difference. Explain the difference between percent error and percent difference. Question 4 The mass of a certain sample of material is 35.00 ±
0.5 g. Its volume is 15.0 ±
0.1 cm
3
. Calculate the density and the percent uncertainty of the density. Show all steps. Question 5 Calculate the variance and the standard deviation of the following test scores: 72, 75, 80, 86, 90. Show all steps in the calculations.
12 Lab Procedure Each group of students will collect and analyze data by performing a series of kinematic experiments. By the end of the lab, students should be able to collect and analyze data, perform calculations involving experimental error, uncertainty, standard deviation, and perform graphical analysis. All PCCC students have free access to Microsoft Office which includes Excel. Materials Needed: 1-m track, PASCO Fan Cart, PASCO Dynamic Cart, timer, Cart launcher
•
The stopwatch has an uncertainty of 10.0 milliseconds. •
The meter stick has gradations of one millimeter. Part 1 Step 1) Gather the needed materials for the experiment and lay them out on your bench. Step 2) Place the cart bumper at the zero (0 cm) mark on the track. Step 3) Push the cart and record the distance traveled and the elapsed time. Record this in Table 1. Step 4) For each of the remaining trials, the cart needs to be pushed so that it travels a greater distance. Record the distance and time for each trial. Be especially careful to make sure the cart does not fall off the track. Step 5) Use graphical analysis software to plot the distance the cart traveled as a function of time. Be sure to take the uncertainty of the distance and time into account. Step 6) Use a linear regression tool to plot the best-fit regression line from the data points and determine the slope of line. Step 7) Determine the error between each data point and the regression line. Include these values in your report. Table 1 Distance (m) Distance Unc. (m) Time (s) Time Unc. (s) Part 2 Step 1) Place the cart bumper at the zero mark of the track. Step 2) Use the Cart Launcher to propel the cart forward and measure the total distance the cart travels and the total time. Step 3) Be especially careful not to let the cart drop off the table. Step 4) Repeat Steps 1) and 3) four times for a total of five trials and record this data in Table 2. Your goal is to get the cart to travel a similar distance within a similar elapsed time for each trial. Table 2 Trial # Distance (m) Distance Unc. (m) Time (s) Time Unc. (s) Speed (m/s) 1 2 3 4 5
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13 Step 5) Determine the average speed of the cart. Step 6) Determine the variance and standard deviation of the speed. Step 7) Calculate the error of the average value of the speed. Part 3 Step 1) Place the PASCO Fan Cart bumper at the zero (0 cm) mark on the track. Step 2) Position one student to record the distance the cart travels and another student, with a stop watch, to record the elapsed time. Instructions for the PASCO ME-6977 Fan Cart o
Rotate the fan case until the pointer is aligned with the 0
o
mark. o
Press the POWER button once. This puts the cart in STANDBY mode. Step 3) Set the cart fan speed to MEDIUM, with no pulse duration. Step 4) Press the power button and allow the cart to move until it reaches approximately 100 cm and record the elapsed time. Step 5) Be especially careful not to let the cart drop off the table. Step 6) Perform a total of 5 trials. Record data in Table 3
.
Step 7) Calculate the average velocity of the cart. Table 3 Trial # Distance (m) Time (s) 1 2 3 4 5
14 Part 4 The displacement of a car as a function of time graph is shown below. The initial velocity is zero. Step 1) By analyzing the plot below, determine the acceleration of the car. Step 2) Kinematics tells us that the displacement of an object as a function of time is given by, ࠵?
6
= ࠵?
!
+ ࠵?
!
࠵? +
1
2
࠵?࠵?
#
The starting point of the car is the zero-reference point. The derivative of this expression as a function of time is the velocity of the car. It is not possible to differentiate directly. Step 3) Create a table in which one column is Δ࠵?
and another column is Δ࠵?
. Step 4) Using the provided plot, choose points x
1
, x
2
and t
1
, t
2
which are close to each other. Use these data points to determine the slope of the function. Move left to right, choose more data points, and fill in the table from Step 3. Step 5) Plot the data points from the table. This plot represents velocity as a function of time. Questions 1) What is the difference between percent error and percent difference? Explain. 2) If your work bench was sloped, what type of error would this produce? 3) If a cluster of data has a low standard deviation, what does that tell us about the spread? 4) What does the slope of the distance vs. time plot represent? 5) What is the difference between RMSE, linear regression, and “best-fit”? 6) In Part 3, if the velocity of the car is constant, what is its acceleration? 7) In Part 3, once the car accelerates, is the displacement as a function of time still linear? Explain. Include all data, graphs, tables, calculations, and answers to these questions in the lab report. 0
50
100
150
200
250
300
1
2
3
4
5
6
7
8
9
10
11
12
13
14
Displacement (m
)
Time (s)
Displacement vs. Time
15 Laboratory 2 Free-Fall
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The standard value for the acceleration due to gravity (g) is 9.80 m/s
2
and is assumed constant. In this laboratory, the rate of acceleration due to gravity of a falling object in free-fall will be experimentally determined. By utilizing the equations of kinematics and graphical analysis tools, the standard value of 9.80 m/s
2
will be compared to the experimentally determined value. The force due to gravity pulls objects towards the earth. For the purposes of this course, the rate of acceleration due to gravity is assumed constant with a standard value of 9.80 m/s
2
. This is an average value and varies depending on the location and topography of where measurements are performed. Although this value may vary, it is very reasonable to consider it a constant for the purposes of this lab. As an object falls, its velocity is continually increasing. However, the acceleration of the object remains constant regardless of its mass. In this laboratory a simple free-fall experiment will be conducted to determine the acceleration due to gravity of an object in free-fall. This value will then be compared to the standard value of g. There are many ways to determine the value of g. The method used in this lab utilizes a simple apparatus: two combined meter sticks attached to a steel post. The purpose of this is to allow a longer fall time for the ball. The ball will be released from rest and allowed to hit the ground. Simultaneously, the elapsed time of free-fall will be recorded using a stopwatch. From this data, the acceleration due to gravity can be determined. The value for (g) obtained will likely not be equal to the standard value. This is due to 1) the experiment has inherent errors in it. 2) The ball will experience air resistance, which is not taken into account. 3) Human observational error may occur. Beyond measuring the value of g, this lab will allow you to gain experience collecting data, in particular, how to eliminate anomalous data points. Further insight will be gained by plotting the data as well as working with non-linear functions. From the graph of distance over time, the slope will yield critical information pertaining to the experiment. From kinematics, the equation of motion for vertical displacement can be expressed as, ࠵? = ࠵?
7
+ ࠵?
7
࠵? −
"
#
࠵?࠵?
#
(1) The initial displacement can be chosen as ࠵?
7
= 0
. As long as the object is allowed to freely fall, there is no initial velocity and ࠵?
7
= 0
. Eq. (1) can be rearranged to solve for the acceleration due to gravity. This is left as an exercise necessary for this lab. Notice the negative sign in Eq. (1). This indicates that the object is falling, and the downward direction is taken to be negative.
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16 Laboratory 2-Prelab
Free-Fall
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 What is the standard value for the acceleration due to gravity? Question 2 What is the purpose of the release mechanism? Question 3 How does the mass of an object affect its rate of vertical fall? Question 4 What mathematical function (linear, parabolic, hyperbolic, etc.) should the plot of the velocity of the falling ball as a function of time be?
Question 5 Plot the following function: y(t) = 4.9t
2
and determine the slope and y-intercept. The plot needs to have axes and units. From this function determine the velocity and acceleration as a function of time and plot both functions.
17 Lab Procedure
Materials Needed:
Tape measure, two meter sticks, adhesive tape, stopwatch, ball, release mechanism Step 1) Attach and vertically position two meter sticks together using adhesive tape. Step 2) Attach the meter sticks to the edge of the workbench. Step 3) One student will position the ball close to the ground, parallel to the meter sticks, and prepare to release the ball. Another student will record the elapsed time of fall using the stopwatch. It is recommended to use the release mechanism so that no initial velocity is imparted to the ball. Step 4) At the instant the ball is released, start the stopwatch (unc. = 10 ms). This will require a lot of practice. You are likely to obtain a few anomalous results. Record your data for displacement and elapsed time to the nearest 10 ms. Step 5) For each trial, the ball should be incrementally raised to a new height, released and the elapsed time of fall recorded for a total of ten (10) trials. Be sure to include the uncertainty in your final answer for the average acceleration due to gravity. Step 6) Using graphical analysis software plot the vertical position as a function of the square of elapsed time for the ball. The y-axis scale should have units of cm for higher resolution. Step 7) Plot the velocity and acceleration of the falling ball as a function of time. Explain in your lab report why your average value of (g) is different than the standard value. Discuss observed discrepancies and what may have contributed to this. Step 8)
Plot the vertical displacement of the ball as it fell using the increments of time from Table 1.
Table 1 Step 9)
Calculate the average value of the acceleration due to gravity, its standard deviation and the uncertainty of the mean of g. Questions 1) What does the slope of the plot y vs. t
2
represent? 2) What does human reaction time indicate? Where could this have occurred in this experiment? 3) If the mass of the ball was doubled, how would this affect the acceleration due to gravity? 4) During a free-fall experiment, a solid metal ball and a hollow metal ball are positioned at the same height and released at the same instant. The metal of each ball has the same density. Which ball has a greater inertia? Should the ball with greater inertia fall more slowly than the lighter ball? Include all data, graphs, tables, calculations, and answers to these questions in the lab report. Trial Distance (cm) t (s) t
2
(s
2
) g (m/s
2
) v (m/s) a (m/s
2
)
18 Laboratory 3 Projectile Motion PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The purpose of this lab is to experimentally verify the equations of kinematics for projectile motion as well as to show the relationship between projectile launch angle, initial velocity and horizontal range. This lab will also verify that the horizontal range of a projectile is a function of both its initial velocity initial launch angle. The lab is divided into two parts. For the first part, the initial angle of the launcher will remain constant, while the initial velocity will be varied. From this data, the range of the projected object can be determined as well as other parameters of the trajectory. For the second part, the initial velocity will be constant while the initial angle of launcher will be varied. For each part the measured horizontal range will be compared to the theoretical value. The first necessary step, before the experiments begin, is to determine the initial velocity of the object as it is projected out of the launcher. The initial velocity cannot easily be measured directly. However, by setting the angle of the launcher to zero degrees and measuring the horizontal range of the projectile and the time of flight, the initial velocity can be determined using Eq. 1. The projectile launcher has three initial velocity settings, each of which yields a different initial velocity. For the first part, the initial velocity will be varied, and the angle of the launcher will remain constant. The values of the initial velocity correspond to the three settings on the projectile launcher. Due to the non-zero initial angle, the initial velocity will have both a horizontal and vertical component. The horizontal component remains constant. In order to determine the vertical component of the initial velocity, trigonometry needs to be utilized. If the experiment is carefully performed, it should be observed that the greater the initial velocity, the greater the horizontal range as indicated from Fig. 1 a). The maximum vertical height of the ball can also be determined using Eq. 3 and Eq. 4. The velocity and angle the instant prior to impact can also be determined using Eq. 3. and Eq. 6. For part two, the initial velocity is held constant while the initial launch angle is varied. Notice from Fig. 1 b), how the range varies as a function of initial angle. Using the medium range of the projectile launcher, the angle will be varied, and the time of flight measured. Eq. 1 can then be used to determine the horizontal range. If the experiment is carefully performed, it should be observed that the greater the initial launch velocity, the greater the horizontal range up until 45
o
. Angles greater than this reduce the horizontal range. ࠵? = ࠵?
!(
࠵?
(1) ࠵? =
8
$
%
934 (#;
$
)
=
(2) ࠵?
>
= ࠵?
!>
− ࠵?࠵?
(3) ࠵? = ࠵?
!
+ ࠵?
!>
࠵? −
"
#
࠵?࠵?
#
(4)
࠵?
#
= ࠵?
(
#
+ ࠵?
>
#
(5)
࠵? = ࠵?࠵?࠵?
!"
H
#
!
#
"
I
(6)
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19 Figure 1.
Projectile trajectory range as a function of initial velocity and angle. a) Initial velocity is varied, and the initial angle is constant. b) The initial velocity is constant, and the initial angle is varied. [1]. Figure 2.
Projectile launcher with labels indicating critical features. Caution! Wear safety glasses throughout the experiment.
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20 Laboratory 3-Prelab Projectile Motion
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 What device will be used to secure the launcher to the table? Question 2 How many range settings does the projectile launcher have? Question 3 How will the angle of the projectile launcher be measured? Explain. Question 4 If the initial velocity of a projectile is known, how can we determine its horizontal and vertical components? Question 5 The horizontal distance will be measured between the landing spot and what other specific location on the launcher? Familiarize yourself with the projectile launcher and be aware of the safety precautions using this device. Refer to Fig. 2.
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21 Lab Procedure
Materials Needed: ME-6800 PASCO
Projectile Launcher, c-clamp, ramrod, plastic ball, safety glasses, measuring tape, stopwatch, adhesive tape, carbon paper.
Caution! Wear safety glasses throughout the experiment.
Steps to Determine the Initial Velocity Step 1) Alternate the launchers on each work bench pointed away from the other lab groups. Step 2) Place the launcher at the same horizontal level in which the ball will land and secure down the launcher with the c-clamp, careful as to not overtighten. Step 3) Adjust the launcher using the thumb screw. Step 4) Adjust the launcher to an angle of zero. Use the plumb bob and angle scale guide. Step 5) Place the plastic ball into the launcher and carefully push it into the chamber using the ramrod. Caution! Be careful not to fire the launcher while loading the ball. Step 6) Set the launcher to the short-range position and prepare the stopwatch to record the time of flight. Step 7) Launch the projectile (ball) by pulling back on the hammer using the attached cord and record the time of flight. Step 8) Place a piece of tape at the landing spot. Use carbon paper if available. Step 9) Use a measuring tape to measure the horizontal distance from the launcher (crosshairs) to the adhesive tape or carbon paper, to the nearest 0.1 cm. Step 10) Repeat Steps 5-9 for the medium and long range. Perform a total of three trials for each range. Step 11) Calculate the initial velocity of the projectile for all three ranges. Record the average values. Part 1-Varying ࠵?
࠵?
Constant ࠵?
࠵?
Step 1) Angle the launcher to 45
o
. Step 2) Set the projectile launcher to the short range and fire the launcher. Approximate the landing site by using adhesive tape as a location marker. Step 3) Once the approximate landing location is determined, place (do not tape) one piece of carbon paper on the floor. Step 4) Measure the elapsed time from launch to landing using a stopwatch. Measure the horizontal range with the measuring tape to the nearest 0.1cm. Record this value. Step 5) Repeat Steps 2) through 4) using the medium and long-range launcher settings. Perform three (3) trials for each setting. Fill in data Table 1. Some values will require calculations. Table 1 Constant ࠵?
࠵?
= 45
o
Average Values Short Range ࠵?
!@8A
Medium Range ࠵?
!@8A
Long Range ࠵?
!@8A
࠵?
!(
(m/s) ࠵?
!>
(m/s) Time of Fight(s) Maximum Height (m) Range (m) ࠵?
6(
(m/s) ࠵?
6>
(m/s) ࠵?
6
(m/s) ࠵?
6
(Degrees)
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22 Part 2-Varying ࠵?
࠵?
Constant ࠵?
࠵?
Step 1) Set the initial velocity of the projectile launcher to the medium range. Step 2) Angle the launcher to 15
o
. Step 3) Fire the launcher. Approximate the landing site by using adhesive tape as a location marker. Step 4) Once the approximate landing location is determined, place (do not tape) one piece of carbon paper on the floor. Step 5) Measure the elapsed time from launch to landing using a stopwatch. Measure the horizontal range with the measuring tape to the nearest 0.1cm. Record these values. Step 6) Repeat Steps 2) through 5) with varying angles as indicated in Table 2. Perform three (3) trials for each angle. Using average values from the three trials, fill in data Table 2. Table 2 Constant Velocity (Medium Range) Average Values ࠵?
!
= 15
7
࠵?
!
= 45
7
࠵?
!
= 75
7
࠵?
!(
(m/s)
࠵?
!>
(m/s)
Time of Fight(s)
Maximum Height (m)
Range (m)
࠵?
6(
(m/s) ࠵?
6>
(m/s) ࠵?
6
(m/s) ࠵?
6
(Degrees) For your report discussion: 1) Explain whether the range has increased or decreased now that the projectile is at an angle. 2) Explain any discrepancies between the theoretical and measured values of range in your lab report. Questions 1) Does the mass of the ball have any effect on the range? Explain. 2) Does the horizontal range of the ball increase with increasing initial velocity? Explain. 3) Does the height of the ball increase with increasing initial velocity? Explain. 4) If the height of the launcher is increased, what effect would this have on the final velocity of the projectile? Explain. 5) Why does the range increase with increasing initial angle? Explain. 6) What is the optimal initial angle to obtain maximum horizontal range? Explain. 7) Why does the range decrease for angles greater than the optimal initial angle? Explain. Include all data, tables, calculations, and answers to these questions in the lab report.
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23 Laboratory 4 Newton’s Second Law of Motion
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The objective of this lab is to verify Newton’s Second Law of motion and determine the acceleration of a moving object. For Part 1, a wheeled cart is placed on a horizontal, frictionless track. The cart is tethered to a string which is wrapped around a pulley with a hanging mass on the other end of the string, as shown in Fig. 1 a). By application of Newton’s second law, the acceleration of the cart can be determined while neglecting friction. For Part 2, the same cart will be placed on an inclined, frictionless track. By application of Newton’s second law, the acceleration of the cart can be determined. Figure 1.
Part 1: Cart on a horizontal, frictionless track with a weight hung across a frictionless pulley. Figure 2.
Part 2: Cart on an inclined, frictionless track. When the cart is on the horizontal track a force is needed in order to impart it with acceleration. Ideally, this force should be constant and controllable. This is the purpose of the vertical masses. The force due to gravity on the hanging vertical masses will impart a force on the cord and this tension will pull the cart along the track. The acceleration of the cart can be determined using Newton’s second law of motion.
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24 Laboratory 4-Prelab
Newton’s Second Law of Motion
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 Sketch the free-body diagram for a block resting on a friction-less horizontal surface. Question 2 What is the purpose of placing the track onto the workbench with a few centimeters protruding over the edge of the table? Question 3 When a force is applied to the block, how will you determine its acceleration? Question 4 How is the photogate going to be used in this experiment? Explain. Question 5 How are you going to determine the experimental velocity of the cart when an external force is applied?
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25 Lab Procedure
Materials Needed: Inclined 1-m track, dynamic cart, pulley, mass hanger, masses, inelastic cord, protractor, two photogates, photogate picket fence, balance, track stand Part 1 Step 1) Measure the length of the opaque portion of the picket fence and insert in into the cart. Step 2) Measure the mass of the dynamic cart while the picket fence is inserted. Step 3) Measure the mass of the mass hanger. Step 4) Place a 1-m track onto the lab bench with a few centimeters protruding over the edge of the table. Step 5) Clamp and secure a small pulley to the end of the track protrusion. Step 6) Level the track to keep it horizontal. Add spacers if necessary. Step 7)
Attach one end of a piece of cord (~ 1 m) to the cart, wrap it over the pulley and attach the other end to the mass hanger. Step 8) Hold the cart in position. Step 9) Place the first photogate close to the cart and the second photogate close to the pulley as shown in Fig. 1. Adjust the height of the photogates so that the picket fence can pass through both sensors. Step 10) Measure the distance between the two photogates. Record this as Δx
. Step 11) Set both photogates to GATE mode. Make sure that the MEMORY feature is off. Step 12) Place the back of the cart at a chosen point on the track and hold it steady. Step 13) Press the RESET button on both photogates. Step 14) Release the cart and record the time it takes the cart to pass through both photogates. Make sure that the cart can completely pass through the second photogate. Δt
"
and Δt
#
represent the amount of time it took the cart to pass through photogate 1 and photogate 2 respectively. Be certain that the cart does not fall off the table and the masses do not hit the ground. Step 15) Repeat Steps 12) through 14) by adding small incremental mass to the mass hanger. Step 16) Calculate the experimental velocity of the cart as it passes through each photogate. Step 17) Determine the experimental acceleration of the cart using the experimental data. Step 18) Determine the percent error between the theoretical and experimental acceleration of the cart. Step 19) Record this data in Table 1. Step 20) Plot the experimental acceleration of the block as a function of applied force acting on the cart. Table 1 Added Mass (kg)
Photogate 1 ࠵?࠵?
࠵?
(࠵?)
Photogate 2 ࠵?࠵?
࠵?
(࠵?)
࠵?
࠵?
(m/s) ࠵?
࠵?
(m/s) a (m/s
2
) Experiment a (m/s
2
) Theory % Error
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26 Part 2 Refer to Fig. 2. This is what your experimental setup should look like.
Step 1) Remove the pulley and incline the 1-m track on the workbench using a track stand. Step 2) Measure the angle of incline using a protractor. Step 3) Use the same photogate picket fence from Part 1. Step 4) Place Photogate 1 at the top of the track. Place Photogate 2 near the bottom of the track as shown in Fig. 2. Step 5) Measure the distance between the two photogates. Record this as Δx
. Step 6) Set both photogates to GATE mode. Step 7) Initially place the cart at the top of the track and hold it in place. Step 8) Press the RESET button on both photogates. Step 9) Release the cart and allow it to pass through both photogates. Record the times from each photogate and include this in Table 2.
Δt
"
and Δt
#
represent the amount of time it took the cart to pass though photogate 1 and photogate 2 respectively. Be certain that the cart does not fall off the table. Step 10) Calculate the experimental velocity of the cart as it passes through each photogate. Step 11) Determine the experimental acceleration of the cart using the experimental data. Step 12) Determine the percent error between the theoretical and experimental acceleration of the cart. Step 13) Repeat Steps 7) through 9) increasing the angle of incline as indicated in Table 2. Step 14) Plot the acceleration of the block as a function of the angle of incline. Table 2 Questions 1) How does the mass of the cart affect its acceleration when placed on the horizontal track? 2) Is the tension in the pulley cord the same on both sides? 3) Is the acceleration of the cart the same as the hanging mass? 4) Why might there be discrepancies between the experimental and theoretical values of acceleration? Include all data, graphs, tables, calculations, and answers to these questions in the lab report. ࠵?
(degrees) Photogate 1 ࠵?࠵?
࠵?
(࠵?)
Photogate 2 ࠵?࠵?
࠵?
(࠵?)
࠵?
࠵?
(m/s) ࠵?
࠵?
(m/s) a (m/s
2
) Experiment a (m/s
2
) Theory % Error 10 15
20 25 30
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27 Laboratory 5
Friction Analysis
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The purpose of this lab is to analyze friction and quantify the effect it has on the acceleration of an object. In Part 1 of this lab a block will slide down an inclined track. The track is made of aluminum and the block is made of wood as shown in Fig. 1(a). Each surface appears smooth and polished to the human eye. However, if a microanalysis of the surfaces were conducted using a powerful microscope as shown in Fig. 1(b), the aluminum and wood surfaces would appear rough and jagged as shown in Fig. 1 (c). Figure 1.
(a) Two seemingly smooth surfaces [1]. (b) Powerful microscope [3]. (c) Image of aluminum surface under the microscope [4]. Once the coefficients of static and kinetic friction are experimentally determined, photogates will be used to measure the elapsed time it takes the block to slide down the incline. From this data, the velocity and acceleration of the block can be determined. This can be repeated for multiple angles. Using Newton’s second law of motion, the theoretical acceleration of the block can be calculated and compared to the experimental value of acceleration from the data. In this experiment you will also verify that the acceleration of any object moving down an incline is independent of its mass. Consider an object, such as a wood block, placed on an inclined plane as shown in Fig. 2. The block has some mass m. The weight of the block is indicated as W. When using Newton’s second law of motion a free-body diagram needs to be constructed and the weight resolved into its components. N is the normal force of the track acting on the block. ࠵?
is the angle of incline. The frictional force is f. The frictional force is always opposite to the direction of potential motion. If the block accelerates, the acceleration will be along the surface of the track. This is the x axis. There is no acceleration along the y axis since the block does not move up or down. Verification of force components will be shown in Part 2. Figure 2. Experimental setup for Part 1 of the laboratory. A block is placed on an inclined plane.
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28 If an external force is applied to an object or a force internal to a system, such as gravitational force, which results in no motion of the object, the coefficient of static friction is given by the inequality, ࠵?
D
≤ ࠵?
D
࠵?
(1) For small angles of incline, the block will not move due to the static frictional force between the block and surface. This is shown in the linear portion of the graph in Fig. 3. At the microscopic level, this is due to atomic welds between the two surfaces. At a certain critical angle, ࠵?
-
, the block will have impending motion, in which the block starts to slip, as shown by the equality in Eq. 2. ࠵?
D
= ࠵?
D
࠵?
(2) Interestingly, the coefficient of static friction is only a function of the critical angle. ࠵?
D
= ࠵?࠵?࠵?(࠵?
-
)
(3) If a greater external force or internal system force (gravity in the case of the inclined block) is applied to the block and the block starts to move, the frictional force is kinetic as shown in Eq. 4.
As the block moves down the incline, the atomic welds between the two surfaces, as shown in Fig. 1 a., break apart.
f
k
= ࠵?
E
N (4) From Fig. 2, the greater the angle of incline ࠵?
, the greater the frictional force. When the applied force (or component of weight in this case) reaches a certain threshold, the frictional force becomes independent of the applied force (or component of weight in this case). This is the non-linear portion of the plot shown in Fig. 3. Angles of incline greater than this will lead to the block sliding down the inclined surface with acceleration. The greater the angle of incline, the greater the acceleration of the block. If the expression for the coefficient of kinetic friction has the same form as Eq. 3, then as the angle of incline increases, the coefficient increases. At first, this does not make any sense because the coefficient of kinetic friction remains constant. Instead, consider a critical angle ࠵?
-
F
which is less than the critical angle ࠵?
-
, as shown in Eq. 5. In other words, once an object is in motion, it is easy to keep it in motion. Figure 3. Plot of the frictional force as a function of the applied force acting on an object [5]. ࠵?
-
F
< ࠵?
-
(5) The coefficient of kinetic friction can then be expressed as, ࠵?
E
= ࠵?࠵?࠵?(࠵?′
-
)
(6)
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29 For Part 3 of this lab, the effects of motion will be studied when the resistance of the medium in which the object is moving is not neglected. For example, when and object such as a ball falls through a gas, such as air, there exists a force which resists this flow of motion, as shown in Fig 4. This force is called air drag or simply the resistive force. If the object is not moving too fast, then the resistive force in which the air exerts on it is given by, ࠵? = −࠵?࠵?
(7) Figure 4.
(a) An object falling through medium with resistive forces [5].
Where b is a constant based on the properties of the medium and the geometry of the object. It is called the drag coefficient. ࠵?
is the velocity of the object relative to the air. Just as with frictional forces, this resistive force is in the opposite direction of the motion of the object. The longer the object is falling in the medium, the greater the magnitude of the resistive force. When the magnitude of this resistive force is equal to the weight of the object, the total (net) force acting on the object is zero. The velocity of the object has reached its terminal velocity. The relationship between this terminal velocity, b, and time is given by Eq. 8. ࠵?
G
is the terminal velocity. ࠵? =
2A
,
m1 − ࠵?
.,H/2
o = ࠵?
G
m1 − ࠵?
.,H/2
o
(8)
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30 Laboratory 5-Prelab Friction Analysis
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 Sketch the free-body diagram for a block on an inclined plane with friction. Question 2 Use Newton’s second law of motion to determine an expression for the acceleration of the block as it slides down the incline. Be sure to include friction. Question 3 What do the expressions ࠵?
D
≤ ࠵?
D
࠵?
and ࠵?
D
= ࠵?
D
࠵?
represent? Explain. Question 4 What does the angle represent in the equation ࠵?
6
= ࠵?࠵?࠵?(࠵?′
-
)
? Explain. Question 5 How high above the ground will the filter be placed?
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31 Lab Procedure
Materials Needed: inclined track, track stand, wood block, protractor, photogates, photogate picket fence, force sensor, balance, adhesive tape, coffee filter, meter stick Part 1 Step 1) Place the track on a steel track support as shown in Fig. 2. Step 2) Incline the track so that the block begins to slip so that it has impending motion. Step 3) From visual observations, determine the critical angle of impending motion. Measure this angle using a protractor. Step 4) Use equation 3 to calculate the coefficient of static friction. Step 5) Increase the angle of incline of the track until the block moves. While the block is sliding down the track, reduce the angle of incline until the block begins to slow down and expression 5 is verified. This is ࠵?′
-
.
Step 6) Use equation 6 to calculate the coefficient of kinetic friction. Step 7) Complete Table 1. Table 1 ࠵?
-
࠵?
D
࠵?′
-
࠵?
E
Step 8) Use adhesive tape to attach the picket fence to the block. The blue portion of the fence must be facing up. Step 9) Place the first photogate near the top of the track and the second photogate close bottom of the track. Adjust the height of the photogates so that the picket fence can pass through both sensors. Step 10) Measure the distance between the two photogates. Record this as Δx
. Step 11) Set both photogates to GATE mode. Make sure that the MEMORY feature is off. Step 12) Place the block near the top of the track and hold it steady. Step 13) Press the RESET button on both photogates. Step 14) Release the block and record the time it takes the block to pass through both photogates. Make sure that the block can completely pass through the second photogate. Refer to Lab 4 on how to calculate the velocity of the block. Step 15) Repeat Steps 12-14 with increasing angles of incline. The angles must be greater than the critical angle to ensure constant acceleration of the block. For each angle, use the data to calculate the acceleration of the block and compare these values of acceleration to the theoretical values of acceleration obtained using Newton’s second law of motion. Complete Table 2. Table 2 ࠵?
(degrees) Experimental
Acceleration
Theoretical Acceleration % Difference
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32 Part 2 Step 1) To verify that the weight of the block (or any object) can be resolved into components, a force sensor will be used. Turn the force sensor ON. Step 2) Calibrate the force sensor by pressing the ZERO button when no weight is applied. Step 3) Assemble the force sensor as shown in Fig. 4 using the largest angle of incline from Table 2. Compare the measured component of weight to the theoretical value. Figure 5. Experimental setup used to measure the components of weight with a force sensor. Part 3
Step 1) Measure the mass of the coffee filter. Step 2) Vertically position the filter 2.0 m from the ground and release it with no initial velocity. Step 3) Measure the distance and time required for the filter to reach its terminal velocity. Step 4) Repeat Step 1 through 3 for a total of three (3) trials. Complete Table 3. Table 3 Trial t (s)
࠵?
G
(m/s) ࠵?
(m/s) Questions 1) Use Newton’s Second Law of motion to show that the acceleration of the block sliding down an inclined plane is independent of its mass. Show all steps. 2) Once the track is inclined to the critical angle, the block begins to slip. As the angle is increased, the block slides down the track. While the block is in motion, the angle of incline is decreased. Will the block continue to slide? Explain. 3) Can the coffee filter be considered a particle under a net force? Explain. 4) What is the average time it took the filter to fall? 5) If air resistance was neglected how long would it take the filter to fall? Compare these values of time to those measured in Table 3. Include all data, tables, calculations, and answers to these questions in the lab report.
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33 Laboratory 6 The Conservation of Mechanical Energy
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The purpose of this lab is to verify the conservation of mechanical energy. We will be using a double-sloped track and a steel ball. Initially positioning the ball to a height h
2
transfers gravitational potential energy to the ball. The ball will roll down the track, pass through the bottom (dotted line) and roll back up to the other side of the track to some height h
3
. Due to friction between the track and the ball, the height h
3
will not be the same as h
2
. The conservation of mechanical energy will be used to determine the velocity of the ball when it is at the bottom of the track. Figure 1.
Double track indicating three critical positions of the ball. The conservation of mechanical energy can be expressed as, Δ࠵?࠵? + Δ࠵?
A
+ ࠵?
5-
= ࠵?
J(H
(1) KE is the kinetic (motional) energy an object has as it moves with some velocity. U
g
is the gravitational potential energy due to an object’s position relative to some reference point. W
nc
is the work done against non-conservative forces, friction for example. Friction between the two surfaces increases the total amount of work needed to change the kinetic energy of the system. W
ext
is external work done on the system due to an external force. Substituting the appropriate equations into each term gives us, "
#
࠵?࠵?
6
#
−
"
#
࠵?࠵?
!
#
+ ࠵?࠵?ℎ
6
− ࠵?࠵?ℎ
!
+ ࠵?
5-
= ࠵?
J(H
(2) For this lab, external forces, though necessary to supply the system with initial energy, will not be taken into account in the calculations, so the last term in Eq. 2 can be neglected. Work is the product between force and distance; therefore, the non-conservative work can be expressed as, ࠵?
5-
= ࠵?
E
࠵? = ࠵?
E
࠵?࠵?
(3) N is the normal force opposing the weight of the object. The expression for this can be determined using Newton’s second law. When the ball is placed on the bottom of the track, it quickly reaches an equilibrium state and has no motion. This also means that there is no energy in the ball-track system. An external force is required to give the ball some initial energy. In order to visualize the motion of the ball as it rolls along the track, the initial energy supplied to the ball will be gravitational potential energy.
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34 Laboratory 6-Prelab The Conservation of Mechanical Energy
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 Where on the double-sloped track will the motion sensor be placed? Question 2 Write down the conservation of mechanical energy and briefly explain each term. Question 3 What is the difference between kinetic energy and gravitational potential energy? Question 4 How is the ball going to be given its initial energy? Question 5 Does the distance (d) represent the height of the track or the distance the ball traveled along the track?
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35 Lab Procedure
Materials Needed:
Double-slopped track, steel ball, meter stick, motion sensor, balance, protractor Steps Step 1) Gather the needed materials and securely set up the double-inclined track. Step 2) Measure the mass of the steel ball. Step 3) Record the angle of incline for both sides of the track. The angles should be equal. Step 4) Place the motion sensor at the bottom of the track. Step 5) Raise the ball up to a height near the top of the right side of the track. Record this as h
2
. Step 6) Gently, with no initial velocity, release the ball and allow it to roll down the track. Step 7) Record the velocity of the ball at the bottom of the track. This is ࠵?
K"
. Step 8) Record the height the ball reaches on the opposite side of the track. Record this as h
3
. Step 9) Perform a total of three trials. Step 10) Look up the value for ࠵?
E
for the steel ball and aluminum track. Step 11) Use the conservation of energy to determine the velocity of the ball ࠵?
K"
when it reaches the bottom of the track. Step 12) Complete tables one through three. Include these tables in your report. Step 13) Compare the calculated velocity of the ball at the bottom of the track with value measured with the motion sensor. Step 14) For each trial, determine the loss of energy of the ball as it moves up to position h
3
. Table 1 m
Ball
(kg) ࠵?
"
(degrees) ࠵?
#
(degrees) ࠵?
E
Table 2 Trial h
1
(m) h
2
(m) h
3
(m) d (m) Table 3 Trial Ug
1
(J) Ug
2
(J) Ug
3
(J) ࠵?
K"
(m/s) ࠵?
K#
(m/s) ࠵?
KL
(m/s) N
(N) W
nc
(J) Questions 1) Does the conservation of mechanical energy hold? If it does not, discuss any discrepancies. 2) Is the height the ball reaches on the opposite side of the track the same as its initial starting position? 3) If the answer to question 2) is no, then explain why. 4) After the ball has been raised up, it is released and passes through the bottom of the track. Can the velocity of the ball at the bottom of the track be determined using Newton’s Laws of motion? Explain. 5) What is the percent difference between the calculated and measured values of ࠵?
K"
? 6) Was there a loss of energy of the ball? If so, what was this energy transformed into? Include all data, tables, calculations, and answers to these questions in the lab report.
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36 Laboratory 7 The Conservation of Linear Momentum
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction This laboratory experiment will demonstrate and verify the conservation of linear momentum. This fundamental principle states that the total momentum of a system remains constant. In this lab, a series of collision experiments will be performed to demonstrate this principle. The mass of each object is known, and the velocities can be measured before and after the collision. According to the conservation of linear momentum, the total momentum of the system prior to the collision is equal to the total momentum of the system after the collision if no other external forces are present. The objects in question are two collision carts. These are specially designed wheeled carts with spring-loaded bumpers to absorb the impact of the collision. These springs also ensure us that the collision remains elastic. The masses of these carts are known. For all parts of this lab, the unknown variable can be solved using the conservation of linear momentum which can be expressed as, ࠵?
",!
+ ࠵?
#,!
= ࠵?
",6
+ ࠵?
#,6
(1) The subscripts indicate the specific cart and the initial and final state. This expression can be written in terms of mass and velocity. Note that the initial and final subscripts only apply to the velocities since the mass of each cart remains constant. Also notice that friction is being neglected. ࠵?
"
࠵?
",!
+ ࠵?
#
࠵?
#,!
= ࠵?
"
࠵?
",6
+ ࠵?
#
࠵?
#,6
(2) An elastic collision is one in both the linear momentum and the kinetic energy is conserved. The conservation of energy for our two-cart system can be written as, "
#
࠵?
"
࠵?
",!
#
+
"
#
࠵?
#
࠵?
#,!
#
=
"
#
࠵?
"
࠵?
",6
#
+
"
#
࠵?
#
࠵?
#,6
#
(3) Eq. 3 can be used to calculate the energy lost in the two-cart system. For example, even though friction is being neglected in the calculations, there is still a loss of energy outside of the system due to friction between the wheels of the carts and the track. During an inelastic collision, the linear momentum is conserved but the kinetic energy is not. For a perfectly inelastic collision, the total linear momentum is still conserved as shown in Eq. 4. After a perfectly inelastic collision the carts will remain stuck together and move with some final velocity. In order to determine the final velocity of this new combined cart system, the masses of each cart can be added together, and the final velocity can be determined using Eq. 5. d࠵? = 0 → ࠵?
!
= ࠵?
6
(4) ࠵?
"
࠵?
"!
+ ࠵?
#
࠵?
#!
= (࠵?
"
+ ࠵?
#
)࠵?
6
(5)
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37 Laboratory 7-Prelab
The Conservation of Linear Momentum
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick
Question 1 What is the purpose of today’s lab? Question 2 Does the total momentum of a closed system remain constant? Question 3 What is the difference between an elastic and inelastic collision? Question 4 Sketch a simple one-dimensional elastic collision and show the direction of the momentum for each object before and after the collision. Question 5 How are you going to experimentally determine the initial and final velocity of each cart?
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38 Lab Procedure
Materials Needed:
Track, two dynamic carts, photogates, photogate picket fence, balance, tape Figure 1. Part 1 experimental setup of the dynamic carts, photogates, and track. Part 1: Cart 1 Moving, Cart 2 at Rest
For Part 1, prior to the elastic collision, Cart 1 will be pushed along the track and move with some initial velocity. Cart 2 will initially be as rest. After the collision, Cart 1 will be moving with a new velocity and Cart 2 will now have a non-zero velocity. Each cart has the same mass. Step 1) Measure the length of the opaque portion of the picket fence and insert in into both carts. Step 2) Place each cart with the spring-loaded bumpers facing each other. Step 3) Setup the experiment to follow Fig. 1. Make sure to place each dynamic cart away from the photogate sensors. Step 4) Using adhesive tape, label each dynamic cart as: Cart 1 and Cart 2. Step 5) Set both photogate timers to GATE mode, press RESET, and turn on the MEMORY feature. When the MEMORY feature is selected, the first displayed time t
i
is when an object initially passes through the photogate before the collision. When the object passes through the photogate a second time, after the collision, the time t
f
is stored in the memory of the photogate. The screen will display the sum of the times. When READ is pressed it provides the sum t
i
+ t
f
. Step 6) While making sure that Cart 2 is at rest, push Cart 1 so that it collides into Cart 2. Make sure to push Cart 1 with enough force so it completely passes through the first photogate and Cart 2 completely passes through the second photogate. Step 7) Use Eq. 1 to determine if linear momentum was conserved. Step 8) Use Eq. 3 to calculate the energy that is lost to friction between the two carts and track. Table 1 Cart 1 mass (kg) Cart 2 mass (kg) t
1i (s) t
2i (s)
t
1f (s)
t
2f (s)
v
1, i
(m/s)
v
2, i
(m/s)
v
1, f
(m/s)
v
2, f
(m/s)
p
i (kg
∙
m/s) p
f (kg
∙
m/s) Energy Loss (J) For all parts, calculate the initial and final momentum and explain whether or not the conservation of momentum is validated.
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39 Part 2: Cart 1 Moving, Cart 2 Moving
For Part 2, prior to the elastic collision, Cart 1 will be pushed along the track and move with some initial velocity. Cart 2 will also be pushed along the track to move with some initial velocity. After the collision, Cart 1 and Cart 2 will now be moving with some velocity slower than the initial velocity. Figure 2. Part 2 experimental setup of the dynamic carts, photogates, and track. Step 1) Locate each cart at opposite ends of the track as shown in Fig. 2. Place each cart with the spring loaded bumpers facing each other. Make sure there is enough space between the photogates so that both carts can fit. Step 2) Set both photogate timers to GATE mode, press RESET, and turn on the MEMORY feature. Step 3) Push Cart 1 and Cart 2 so that they collide. Make sure to push each cart with enough force so they completely pass through the photogates. Step 4) Use Eq. 1 to determine if linear momentum was conserved. Step 5) Use Eq. 3 to calculate the energy that is lost to friction between the two carts and track. Table 2 Cart 1 mass (kg) Cart 2 mass (kg) t
1i (s) t
2i (s)
t
1f (s)
t
2f (s)
v
1, i
(m/s)
v
2, i
(m/s)
v
1, f
(m/s)
v
2, f
(m/s)
p
i (kg
∙
m/s) p
f (kg
∙
m/s) Energy Loss (J) Part 3: Cart 1 Moving with Added Mass, Cart 2 at Rest This part is similar to Part 1 with the modification that Cart 1 will have some additional mass added to it. Step 1) Place a mass bar on top of Cart 1 and place Cart 2 at rest following Fig. 1. Make sure to place each dynamic cart away from the photogate sensors. Step 2) Place each cart with the spring-loaded bumpers facing each other. Step 3) Set both photogate timers to GATE mode, press RESET, and turn on the MEMORY feature. Step 4) While making sure that Cart 2 is at rest, push Cart 1 so that it collides into Cart 2. Make sure to push Cart 1 with enough force so it completely passes through the first photogate and Cart 2 completely passes through the second photogate. Step 5) Use Eq. 1 to determine if linear momentum was conserved. Step 6) Use Eq. 3 to calculate the energy that is lost to friction between the two carts and track.
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40 Table 3 Cart 1 mass (kg) Cart 2 mass (kg) t
1i (s) t
2i (s)
t
1f (s)
t
2f (s)
v
1, i
(m/s)
v
2, i
(m/s)
v
1, f
(m/s)
v
2, f
(m/s)
p
i (kg
∙
m/s) p
f (kg
∙
m/s) Energy Loss (J) Part 4: Cart 1 and Cart 2 Moving with the Same Velocities Step 1) Remove the mass bar. You can continue to use the photogates or manually measure the velocity of each cart prior to the collision. Step 2) Locate each cart at opposite ends of the track. Place each cart with the spring-loaded bumpers facing each other. Press in and lock the springs. Step 3) At the same time, push both carts towards each other. Try to apply the same force to each cart so that each cart acquires the same velocity. Record the distance and time of travel prior to the collision. Step 4) Both carts should have stopped at the same point and have zero velocity. Table 4 Cart 1 mass (kg) Cart 2 mass (kg) t
1i (s) t
2i (s)
t
1f (s)
t
2f (s)
v
1, i
(m/s)
v
2, i
(m/s)
v
1, f
(m/s)
v
2, f
(m/s)
p
i (kg
∙
m/s) p
f (kg
∙
m/s) Energy Loss (J) Hint:
When applying the conservation of linear momentum, one of the carts will have a negative velocity, be sure to include this in the calculations. Questions 1) Is momentum conserved during an elastic collision? Explain. 2) Is kinetic energy conserved during an elastic collision? Explain. 3) Is momentum conserved during an inelastic collision? Explain. 4) Is kinetic energy conserved during an inelastic collision? Explain. 5) When this experiment is performed in the lab the initial and final kinetic energies during an elastic collision are not equal. Does this violate the conservation of mechanical energy? Explain. 6) If Part 1 was repeated with the track inclined to some angle, would the conservation of linear momentum still hold? Explain Include all data, tables, calculations, and answers to these questions in the lab report.
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41 Laboratory 8 The Ballistic Pendulum
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The ballistic pendulum is a commonly used laboratory apparatus to demonstrate the conservation of linear momentum. An object, in this case a plastic ball, is horizontally fired with some initial velocity into a pendulum. At impact, the pendulum swings upward as shown in Fig. 1. The pendulum reaches some height (h) depending on the momentum of the ball. The maximum height (h) in which the pendulum rises depends on the initial kinetic energy of the ball. The usefulness of this is that we can determine the initial velocity of the ball without directly measuring it. Refer to Fig. 1 below. The mass (m) is the mass of the ball. After impact, the mass is combined with the block as labeled (M + m). The pendulum bob swings upward to a height (h). It is easiest to think of this experiment in two parts: 1) The ball and pendulum are combined into one system during an inelastic collision and moves with some initial kinetic energy (KE). 2) This kinetic energy is transformed into gravitational potential energy (PE
g
) as the pendulum swings upward to a height (h). (a)
(b)
Figure 1. a) Image: PASCO 6831 Ballistic pendulum and launcher [6]. b) Schematic of the ball being fired into the ballistic pendulum.
Once the ball impacts the pendulum, the ball-box system moves as one mass with the same velocity. ࠵?࠵?
7
= (࠵? + ࠵?)࠵?
6
(1) After the collision, the ball-box system moves upward to a height (h). From the conservation of mechanical energy, the initial KE is transformed into PE
g
. "
#
(࠵? + ࠵?)࠵?
6
#
= (࠵? + ࠵?)࠵?ℎ
(2) We can solve for ࠵?
7
simply by measuring the height (h) of the pendulum.
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42 Laboratory 8-Prelab The Ballistic Pendulum
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 What is the purpose of a ballistic pendulum? Question 2 What device will be used to measure the velocity of the projectile? Question 3 What is the purpose of the ramrod? Question 4 When the projectile embeds itself into the block and the block swings upward, what transformation of energy has taken place? Question 5 To solve for the initial speed of the projectile it is necessary to divide the problem up into two parts. Explain why.
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43 Lab Procedure
Materials Needed:
Safety glasses, projectile launcher, PASCO 6831 ballistic pendulum, ballistic ball, ramrod, motion sensor, balance Steps Step 1) Measure and record the mass of the ball. Step 2) Place the ballistic pendulum on the workbench. Be sure that it is not facing towards other lab groups. Step 3) Carefully raise up the pendulum and secure it there. Step 4) Put on safety glasses and load the ball into the launcher using the ramrod. Step 5) Set the launcher to the lowest setting. Be careful to not place your fingers into the chamber. Step 6) Place the motion sensor in front of the launcher to record the velocity of the ball. Step 7) Aim and launch the ball so that it passes through the motion sensor. Do not look directly into the muzzle. Record the initial velocity of the ball from the motion sensor. Step 8) Repeat Step 7 for a total of three trials. Step 9) Load the ball into the launcher using the ramrod. Set the launcher to the lowest setting. Be careful to not place your fingers into the chamber. Step 10) Carefully lower the pendulum until the rubber stopper touches the muzzle chamber. Do not look directly into the muzzle. Aim and launch the ball into the pendulum. Step 11) Record the height of the ball-pendulum system relative to its initial position. Step 12) Repeat Steps 9 through 11 for a total of three trials. Step 13) Calculate the theoretical value of the initial velocity of the ball. Step 14) Determine the percent error between the theoretical initial velocity of the ball and the value obtained from the motion sensor. Questions 1) What type of collision was this? 2) Was linear momentum of the system conserved? Explain. 3) Was kinetic energy of the system conserved? Explain. 4) How accurate was the experimental value of the initial velocity as compared to the calculated value? 5) Calculate the amount of energy that was lost during the transformation from kinetic to gravitational potential energy. Include all data, calculations, and answers to these questions in the lab report.
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44 Laboratory 9
Uniform Circular Motion
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction In this laboratory uniform circular motion (UCM) will be studied and Newton’s Second Law for centripetal acceleration and centripetal force will be verified. In Part 1, a plastic ball will be attached to a spring and a cord and rotated in UCM. Since the spring constant and displacement of the spring can easily be determined, the centripetal force can be calculated. From this, the tension in the cord can be determined. In Part 2, a ball and looping-the-loop track will be used to demonstrate circular motion. In Part 3, non-uniform circular motion will be studied. When an object rotates in a circle with constant velocity, this type of motion is called uniform circular motion. Consider a ball, which can be approximated as a particle, on a string rotating in a circle. Newton’s Second Law of motion still holds; however, the acceleration of the ball is given by the expression as shown in Eq. 1. Where v, is the tangential velocity of the ball and r is the radius of the circle. Substituting this back into Newton’s Second Law gives us Eq. 2. Since direct measurements of the tension of the string would be difficult a spring can be used to determine the centripetal force acting on the string. Hooke’s law is given by Eq. 3. From Eq. 3, ࠵?
is the spring constant and x is the displacement of the spring. This is the amount the spring has stretched from its equilibrium position. The negative sign is the restoring force of the spring. Note that if the spring is displaced in the y-direction, just replace x with y. ࠵?
-
=
8
%
N
(1) Σ࠵?
-
= ࠵?࠵?
-
=
28
%
N
(2) ࠵?
⃗
= −࠵?࠵?
⃗
(3) A plastic ball will be attached to a spring and a cord and rotated in UCM, as shown in Fig. 1. The spring constant of the spring is not known but can be determined by measuring the displacement of the spring and applying Hooke’s law. Figure 1.
Diagram for the ball-spring system indicating the displacement of the spring.
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45 Laboratory 9-Prelab Uniform Circular Motion
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 What is the purpose of today’s experiment? Question 2 During uniform circular motion, which quantity remains constant? Question 3 Sketch the free-body diagram of a ball attached to a string and rotating in uniform circular motion. Question 4 How are you going to determine the spring constant of the spring? Question 5 Write and label each part of Hooke’s law.
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46 Lab Procedure
Materials Needed:
Plastic ball, cord, spring, mass hanger, meter stick, balance, safety glasses, tape, looping-the-loop track Steps-Part 1
Step 1) Measure and record the mass of the plastic ball using a balance. Step 2) Measure and record the mass of the mass hanger. Step 3) Vertically position the spring on the table. Step 4) Connect a mass hanger to the spring and wait until the system reaches equilibrium. Step 5) Displace the mass hanger and record its displacement. Step 6) Calculate and record the spring constant (Eq. 3). Since the spring is vertical, x is y. Step 7) Remove the mass and securely attach the plastic ball to a piece of cord. Step 8) Attach the other end of the cord to the spring. Attach another piece of cord to the other end of the spring. This is the end in which the system will be rotated. Step 9) Measure and record the radius of the system before the spring is displaced. Safety: Keep a safe distance away from the rotating system. Be aware that the spring is going to stretch considerably. Rotate the system away from yourself and other lab members. Step 10) Gradually begin to rotate the spring-ball system until UCM is achieved. Step 11) Measure and record the displacement of the spring while it is in UCM. Step 12) Determine the centripetal acceleration and tangential velocity of the ball. Step 13) Determine the centripetal force acting on the ball and the tension in the cord. Steps-Part 2
Step 1) Position the ball at the top of the looping-the-loop track and record this height. Step 2) Place a motion sensor at the bottom of the track. Step 3) Release the ball with no initial velocity. Observe how the ball completes a full revolution around the loop without falling from the track. It may take a couple of attempts for this to be successful. You may need to adjust the initial height of the ball. Step 4) Record the velocity of the ball at is passes through the motion sensor. Step 5) Calculate the velocity at the top of the track, and the normal forces at the bottom and top of the track. Steps-Part 3
When the velocity of the ball is no longer constant, the circular motion is no longer uniform. The total acceleration on the ball is now the sum of the tangential component and the radial component, ࠵?
~⃗ = ࠵?
~⃗
N
+ ࠵?
~⃗
H
(4) The total centripetal force acting on the ball is, Σ࠵?
~~⃗
= ࠵?
~~⃗
N
+ ࠵?
~~⃗
H
(5) Step 1) On a circle, sketch the components of the total acceleration from Eq. (4) Step 2) Sketch the components of the total centripetal force acting on the ball from Eq. (5).
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47 Questions 1) What keeps the ball in uniform circular motion?
2) In what direction would the ball fly off at if the cord broke? 3) Sketch a circle with radius, r, and indicate the directions of centripetal acceleration, tangential velocity, centripetal force and tension of the ball as it rotates with UCM. 4) What is the magnitude of the tangential component of the acceleration? 5) In Part 2, calculate the minimal height that the ball could be released from and still loop-the-loop. 6) In Part 3, what could have caused this additional tangential component of acceleration to act on the ball? Will this component have any effect on the radial component of acceleration? Explain. Be sure to include all diagrams, data, calculations, and answers to these questions in your lab report.
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48 Laboratory 10 Rotational Dynamics
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction In this lab we will explore rotational dynamics for two systems. In Part 1, an Atwood machine will be constructed with two unequal masses wrapped over a pulley. The translational velocity of the system can be determined by applying the conservation of mechanical energy. For Part 2, two objects of equal mass will be rolled down an incline. One object is solid and the other hollow. It is not intuitive as to which one wins the race to the finish line. Using the conservation of mechanical energy and rotational dynamics, the angular and translational velocities can be determined for each object. Part 1: The Atwood machine Fig. 1. is an illustration of an Atwood machine. Two unequal masses are wrapped over a pulley. The friction between the axis and the pulley is neglected. Assume there is no slippage between the cord and the pulley. When this is the case, the two connected masses move with the same acceleration. If no external forces act on the system, the system is isolated. With no external forces and friction neglected, the conservation of mechanical energy is, Δ࠵?࠵? + ࠵?࠵?
A
= 0
(1) The initial and final kinetic and potential energies of each object must be taken into account. This also includes the pulley. Figure 1. Atwood Machine Part 2: Rolling Down a Hill
From Fig. 2 we see a sphere at the top of an inclined plane. In this lab, two spheres will be used, one solid, the other hollow. Both start at the same location at the top of the incline. Which sphere will win the race and reach the bottom of the incline first? It is easiest to solve this problem using energy considerations. When the spheres are placed at the top of the inclined plane, they each have gravitational potential energy. When they are released and roll down the plane, this energy is transformed into kinetic energy. Since the sphere is rotating there is also rotational kinetic energy present. Figure 2.
Sphere rolling down and inclined plane. Depending on how much friction there is between the surface of the plane and spheres determines whether they roll, slip, or both. We will assume there is some friction present. This implies that they will roll and most likely slip a little as well. Both translational and rotational kinetic energy are present. To best understand the three possibilities of rotation of an object, refer to Fig. 3. When there is no translational motion, the object moves with pure rotation, as shown in Fig. 3a. The only velocity present is angular velocity. If one were to observe the center of mass of the object, they would notice no translational motion. If there is slippage between the ball and the surface, e.g., car tires on ice, as shown M
2
M
1
M
2
M
1
h
h
R
M
M
!
M
!
⃗
!"
!
⃗
!"
#
#
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49 in Fig. 3b. If there is both rotational motion and a bit of slippage, then the translational motion of the object is a combination of these two types of motion. Figure 3.
An object moving with a) pure translation, b) pure rotation, c) both rotational and translational motion. When each sphere is at the top of the incline it has some initial gravitational potential energy. As each sphere rolls down the incline, its initial gravitational potential energy is transformed into both rotational kinetic energy and translational kinetic energy. The parallel axis theorem can be used to determine the moment of inertia of the point P some distance R from the center of mass of the sphere. ࠵?
O
= ࠵?
-2
+ ࠵?࠵?
#
(2) ࠵?
-2
is the moment of inertia of the center of mass of the sphere. ࠵?࠵?
#
is the moment of inertia at a point some distance R from the center of the sphere. The total kinetic energy of the sphere is the sum of the kinetic energy of the translational motion and the kinetic energy of the rotational motion. ࠵?࠵? =
"
#
࠵?
-2
࠵?
#
+
"
#
࠵?࠵?
#
࠵?
#
(3) It is much easier to measure the translational velocity than the angular velocity. Substitute ࠵? = ࠵?
-2
/࠵?
into Eq. 3. Where ࠵?
-2
is the velocity of the center of mass of the sphere. ࠵?࠵?
N
=
"
#
࠵?
-2
°
8
&!
P
²
#
+
"
#
࠵?(࠵?
-2
)
#
(4) The conservation of energy can now be applied to the sphere. Once the terms are placed into this expression, the translational velocity can be determined. This value can then be compared to the measured value. Once the translational velocity is determined, the translational acceleration of each sphere can also be determined. Hint: use an expression from kinematics. !"
P
P
C.M.
C.M.
C.M.
#
!"
!
!"
= 0
!"
P
P
#
!"
#
!"
P
P
# = 0
#
!"
#
!"
+ !"
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50 Laboratory 10-Prelab
Rotational Dynamics
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Question 1 What is the purpose of today’s experiment? Question 2 What is the purpose of having unequal masses on the Atwood Machine? Question 3 How does rotational dynamics differ from uniform circular motion? Question 4 What is the difference between translational and rotational motion? Question 5 How is measuring the radius of each sphere and using the photogate going to allow you to determine the velocity of each rolling object?
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51 Lab Procedure Materials Needed: Track, pulley, two masses, cord, meter stick, balance, solid sphere, hollow sphere, protractor, Vernier caliper, photogate, motion sensor, stopwatch Part 1: The Atwood Machine Step 1) Measure the mass and radius of the pulley. Step 2) Clamp and secure the pulley to a steel post. Step 3) Wrap the cord around the pulley and secure a mass on each end. Make sure that m
1
≠
m
2
. Step 4) Setup and align the photogate so that one of the masses can pass through it. Step 5) Set the photogate to GATE mode. Step 6) Position a meter stick to record the displacement of the masses. Make sure to indicate the initial height reference where h = 0 m. Step 7) Release the system from rest and measure the displaced vertical distance and record the elapsed time from the photogate. Step 8) Use the conservation of mechanical energy to determine the theoretical velocity of the masses. Both masses have the same velocity. Compare this value to the velocity as determined from the experiment. Step 9) Calculate the net torque acting on the pulley. Step 10) Create a table with your results. Label this as Table 1. Show all calculations. Part 2: Rolling Down an Incline
Step 1) Incline the metal track and measure the angle and height. Step 2) Using the Vernier caliper, measure the radius of each sphere. Step 3) Position one photogate at the bottom of the incline. Be sure that the rolling ball will not strike the photogate. Step 4) Set the photogate to GATE mode. Step 5) Place each sphere at the top of the incline. Step 6) Gently release the spheres from rest as to not give them an initial velocity. Step 7) Record the total distance traveled and the elapsed time from the top of the incline to the bottom. Step 8) Record the time measured from the photogate. Step 9) Determine the theoretical values of the velocity of each sphere using the conservation of energy. Include this in the Table as shown below. Step 10) Calculate the measured value of the velocity of each sphere using the measured values of displacement and time. Include this in the Table as shown below. Mass (kg) Radius (m) Distance (m) Time (s) ࠵?
HKJ7N>
(m/s) ࠵?
2J+D.
(m/s) Solid Hollow Questions 1)
Which sphere rolls down faster? Why? 2)
Is the velocity of the solid and hollow sphere independent of its mass and radius? 3)
What happens if we neglect friction as the spheres roll down the plane? Explain. Be sure to include all data, calculations, and answers to these questions in your lab report.
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52 Laboratory 11 Conservation of Angular Momentum PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction If a disk is rotated as shown in Fig. 1 (a), it develops some angular velocity and angular momentum. If you let your right hand represent the spinning disk, the direction of your thumb points in the same direction as the angular velocity and angular momentum shown in Fig. 1 (b). By using the right-hand-
rule we can determine the direction of these quantities for any type of rotating object. The expression for torque is given by Eq. 1. and points in the same direction as angular momentum. Figure 1.
(a) Rotating disk. (b) Right-hand-rule representing the spinning disk. Images: [1]. Σ࠵? =
!࠵?
!#
(1) ࠵? = ࠵? × ࠵?
(2) If a wheel is spun CCW as shown in Fig 1 (a), then by using the right-hand-rule we can determine that the direction of angular velocity and angular momentum points towards her left. If she applies a force downward with her left hand and a force upward with her right hand to rotate the wheel, the resulting motion of it is not intuitive. Using the right-hand-rule, the wheel will have a component of angular momentum towards her, as shown in Fig. 2 b. Since torque also points in the same direction, there will be an additional torque directed towards here as well. This is called gyroscopic precession. Figure 2.
(a) Forces applied to spinning wheel. (b) Vector representation of angular momentum. Images [5].
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53 The purpose of this experiement is to determine the angular precessional velocity of a rotating wheel as a torque is applied. The equation for precessional angular velocity is given by Eq. 3. ࠵?
$
=
%&’
()
(3) r: is the distance from the pivot point to the center of mass. m: is the mass of the wheel. g: is the acceleration due to gravity. I: is the moment of inertia of the wheel. ࠵?:
is the angular velocity of the wheel. The relationship between the precessional angular velocity and the angular momentum using vector notation is given in Eq. 4. ࠵?⃗ = Ω
~~⃗
× ࠵?
~⃗
(4) ࠵?⃗
is the torque acting on the spinning wheel. Ω
~~⃗
is the precessional angular velocity. ࠵?
~⃗
is the angular momentum of the spinning wheel. The period of rotation of the wheel is, ࠵?
$
=
*+
)
&
(5) Interactive Video and Simulation
This laboratory will consist of a series of interactive videos and simulations based on the conservation of angular momentum. The instructions for the lab report format will be explained at the beginning of the laboratory session. It is advisable to review the concepts of the angular momentum and the conservation of angular momentum prior to attending the laboratory.
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54 Lab Procedure
Materials Needed: Bicycle wheel, rotating platform, meter stick. Steps Step 1) Firmly grip the handles on the bicycle wheel prop. Step 2) Have a lab member apply a force perpendicular to the radius of the wheel. Step 3) Observe the motion of the rotation. Step 4) Repeat this now standing on the rotating platform. Step 5) While standing on the platform use your hands to apply perpendicular vertical forces on the handles of the bicycle wheel prop as shown in Fig. 2. Step 6) Observe and record what happens next using the conservation of angular momentum. Questions Presented during the lab session. Be sure to include all calculations and answers to these questions in your lab report.
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55 Laboratory 12 Fluid Dynamics and Heat Exchange
PY-120 Physics I Laboratory Passaic County Community College Professor:
Wayne Warrick Introduction The change in entropy is a thermodynamic state property which relates the amount of energy transferred, either absorbed or expelled from a system. A system could be something as simple as a calorimeter vessel containing water, as will be used in this lab. If energy is either added (absorbed) or removed (expelled) from the system, there is a change in entropy to the system. If energy is absorbed to the system the change in entropy increases and is positive. If energy is expelled from a system, the change in entropy is decreases and is negative. The change in entropy during an infinitesimally (microscopic) small process is defined in Eq. 1. It describes the how the system changes from one equilibrium state to another for an infinitesimal process. dS is the change in entropy of the system. ࠵?
N
is the amount of energy either expelled or absorbed during a reversible (idealized) process. T is the temperature in Kelvin. Since entropy is a state variable if only depends on the initial and final endpoints during a process. If we want the change in entropy for the macroscopic process then we must integrate Eq. 1 from the initial to final states of the process, as shown in Eq. 2. If our system consists of water at some initial temperature placed within an aluminum vessel then the energy required to change the temperature of the water is given by Eq. 3. ࠵?࠵?
N
is the infinitesimal energy change. m is the mass of the substance, water in this case. c is the specific heat of the substance. Since temperature is not really constant for any real process, dT represents the change in temperature as a change in energy occurs in the system. Substituting Eq. 3 into Eq. 4 yields the general expression for the change in entropy of a system during a real, irreversible process. ln is the natural logarithm. Notice how the temperature on depends on the initial and final states. Also, the temperature must be in Kelvin. dS=
dQ
r
T
(1)
ΔS= ³ dS= ³
dQ
r
T
f
i
f
i
(2)
dQ
U
= mcdT
(3)
ΔS = mc ³
dT
T
= mcln -
T
V
T
3
/
V
3
(4)
m: the mass needs to be converted to grams. T: the temperature needs to be converted to Kelvin c: the value for the specific heat of water can be found in the textbook.
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56 Lab Procedure Materials Needed:
PASCO Calorimetry Set, two thermometers, insulating cup, hot and cold water, balance. Figure 1.
(a) PASCO calorimetry setup showing the inner and outer cup, seal ring, and lid. (b) Inner cup with seal ring being inserted into the large outer cup. [7]. Steps Step 1) Use the balance to measure the mass of the inner cup. The larger, outer cup does not change temperature during the experiment. It acts as an insulator and so we do not need its mass. Step 2) Place approximately 30 g of very cold water into the inner cup. Step 3) Use the balance to measure the mass of the cold water and the inner cup. Step 4) Place the spacer over the inner cup as shown in Fig. 1 b. Step 5) Insert the inner cup into the larger cup, as shown in Fig. 1 b. Step 6) Measure and record the temperature of the cold water. Be sure to convert from o
C to Kelvin. Leave the thermometer in the cup. Step 7) Pour approximately 100 g of hot water into the insulating cup and record the initial temperature of the water. Leave the thermometer in the insulating cup for now. Step 8) Remove the calorimeter cup lid and pour about 30 g of the hot water into the inner cup. Step 9) Gently stir the water. Step 10) Place the thermometer (used to measure the temperature of the hot water) into the new mixture of hot and cold water. Step 11) Wait until the two thermometers read the same value. Record the final temperature of the system. Step 12) Use the scale to determine the weight of the final system which consists of the inner cup and the mixture of hot and cold water. Table 1 m
H m
C m
inner T
Hi T
Ci T
i T
f Δ࠵?
W
Δ࠵?
X
Δ࠵?
Questions 1) What does a negative change in entropy represent? What about a positive sign? 2)
Evaluate the sign of the change in entropy for the entire system. Explain in terms of the definition of entropy, and the concept of spontaneous processes. Include the answers to these questions, all calculations, and plot in the lab report.
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57 References [1] Paul Peter Urone, Roger Hinrichs, OpenStax, College Physics, Jun 13, 2022, Houston, Texas, Book URL: https://openstax.org/books/college-physics-2e [2] By M. W. Toews - Own work, based (in concept) on figure by Jeremy Kemp, on 2005-02-09, CC BY 2.5, https://commons.wikimedia.org/w/index.php?curid=1903871 [3] https://www.zeiss.com/microscopy/int/products/stereo-zoom-microscopes/stemi-305.html [4] By Harald Wallin (Haraldwallin) - Own work, Public Domain, https://commons.wikimedia.org/w/index.php?curid=8718968 [5] William Moebs, Samual J. Ling, Jeff Sanny, OpenStax, University Physics Vol. 1, Sep. 19, 2016, Houston, Texas, Book URL: https://openstax.org/details/books/university-physics-volume-1 [6] PASCO 6831 Ballistic Pendulum Launcher [7] PASCO ET-8499 Energy Transfer Calorimeter Manual
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