Spring Constant Report julia

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Athabasca University, Athabasca *

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1007

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Computer Science

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Jan 9, 2024

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docx

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Carleton University Laboratory Report Course #: Experiment #:3 PHYS1007L10 Spring constant JULIA MATAR 101100731 Date Performed: 2023-10-18 Date Submitted: 2023-10-31 Lab Period: 8:30-11:30 Partner: no partner Station #: 24 TA: Matt
Purpose The purpose of the Spring Constant Lab is to work with Hooke’s Law to determine unknown spring constant and learn how to linearize equations using the static method and dynamic method. Static Method: Fig 1: Results of the Static Method 𝑘? , 𝜎𝑘? and the Y-intercept (b). Table 1: : Results of the Static Method 𝑘? , 𝜎𝑘? and the Y-intercept. Slope Y-intercept m σ m b σ b Value 31.38 1.089 0.4157 0.08944 Units N/m N
Dynamic Method: –––– Fig 2: Results of the Dynamic Method 𝑘? , 𝜎𝑘? , the Y-intercept (b), and the Force. Table 2: : Results of the Dynamic Method 𝑘? , 𝜎𝑘? and the Y-intercept. Slope Y-intercept m σ m b σ b Value 0.03318 0.0002608 0.002607 0.0001437 Units kg/ s 2 s 2 Calculations Use templates from previous labs to copy/paste any symbols or equations that you may require to complete this report Hooks law is used to calculate the acceleration due to gravity Fg=Ksx
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Fg=Mg ( k s ±σ k s ) = ( 31.38 ± 1.089 ) N/m t-test= σ ( ¿¿ b 2 + σ b ) 2 = ¿ bp b ¿ KsX=MGx Wheree X is the extension Gx= KsX M = 31.38 ( 0.144 ) 0.4 = 11.3N Dynamic Method Calculations 𝑘 d = 1 m = 1 0.03318 =30.138 kg/s 2 𝜎kd= σ m m 2 = 0.0002608 ( 0.03318 ) 2 =0.235894 kg/s 2 Now to convert it to N/m kg s 2 N = k gm s 2 kg / s 2 m = kg s 2 so k gm s 2 = kg s 2 therefore the two units are equivalent So, ( k d ±σ k d ) = ( 30.138 ± 0.235894 ) N/m
3 ω = σ k d M = 0.310820496 0.55 = 0.75234( side calc) ω av = ω 1 + ω 2 + ω 3 + ω 4 + ω 5 + ω 6 + ω 7 + ω 8 + ω 9 + ω 10 + ω 11 11 = 6.930 rad / s ( side calculation) 1 ω 2 = 1 Kd M + 1 Kd ( M Kd + Mh ) = 1 ω 2 = 1 Kd M + 1 Kd ( b ) 1 ω 2 = 1 30.138 0.03318 + 1 30.138 ( 0.002607 ) = 0.0001187437 rad/s 2 Approx.” 0.00012 rad/s 2 σ 1 / ω 2 = 1 σ k d σ m + 1 σ k d ( σ m σ k d + Mh ) = 1 σ k d σ m + 1 σ k d ( σ b ) = 1 0.235894 + 1 0.235894 ( 0.0001437 ) = 0.0001714753 rad/s 2 Approx.:0.0018 rad/s 2 ( 1 / ω 2 ±σ 1 / ω 2 ) ¿ ( 0.0001187437 ± 0.0001714753 ) N/m Discussion Using the values in Table 1 and 2 the spring constant found through the static method was calculated based on graph to be 31.38 ±1.089 N/m . the calculated result of the y-intercept, the answer was less than 2, making the data consistent. In the dynamic method, by linearizing the equation and finding the slope of the graph, the spring constant was calculated to be ( ( 30.138 ± 0.235894 ) N/m
Experiment Overview During the lab,I determined the spring constant of a spring through the dynamic method and static method . The setup consisted of a LabQuest MINI, a sets of masses weighing from 10g-500g, a motion detector, a spring, and a force sensor. During the stated method I connected the LabQuest MINI interface to the school laptop, I also placed the motion detector to the ground aligning right above the spring and added a metal sheet that would protect the motion detector from the weights that are placed on the spring from falling. I make sure the sensor was placed at zero and then started recording the weight from 50g up to 500g with specific increments added based on the increments needed that was shown on the logger pro.after finishing the static method experiment, the Dynamic method was next. During the dynamic method, there was no need for the LabQuest Mini and I started placing weights on the spring from 600g decreasing to 500g as the lowest mass recorded, with each increment decrease of 10g for this method I was required to pull the wight down and release before recording the oscillation result for each weight. Analysis: Comparison In terms of a more reliable method, I believe that the static method having to have the motion sensor detector for more accuracy it would be a more reliable method because I had to wait for the numbers to be stabilized before recording each mass to determine the spring constant, as for the dynamic method because I am exerting a force that is different each time I change the weight and each force I put on the weight is a different force than the other one, it could create a lot of uncertainties. Moreover, in the dynamic method the mass can sway around side to side and not up and down when I pull the mass which could also give inaccurate results.I was also worried in terms of the accuracy of the both experiments because the object that was holding the weights and was attached to the spring was very uneven and extremely crooked, and it for sure affected my experiment especially during the dynamic method where it kept on swinging from side to side and the weights kept falling. I had to record the dynamic method experiment twice because it was not giving correct results due to the weights falling and spring swaying side to side instead of up and down.therefore,the crookedness of the object that held the weight resulted in the experiments to be not as precises and as accurate as the should be if the object was stable and not crooked Sources of Uncertainty Having a stable straight object to hold the weights that are being placed on the spring and also ensuring that the sensors start at zero at the beginning of the experiments is important if I am looking for more accurate and correct/approximate results. I know for a fact that the dynamic method is not certain and has a higher level of uncertainty than the static method, because it requires an outside force(my hand) to push the spring down to record the Oscillation of the spring which resulted in having inaccurate results, I cannot say the same for the static method, since there was no force applied and since there was a sensor motion detector that was zeroed which also results in certain records, making sure the sensor is set at zero is important for more accuracy. I would say that even if the object that carried the weights was not crooked, the dynamic method will still have a higher source of uncertainty than the static method since the mass did not go down in a perfect vertical position when being pulled and still sway from side to side which will result in not having a perfect vertical motion. Nevertheless, if the
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object object to carry the masses was more straight and less crooked both the results for the dynamic and static method would be more accurate and I will have different recorded results. Improvements In terms of improvements for more certain results and calculations I would suggest to have the object that carried the weights and is placed on the spring, to be a straight vertical object and not a crooked one like the one I had to work with for this lab,I can also say that if there is a stable force to control how the spring is being pushed/ pulled down instead of us pulling it down, it would for sure create more accurate results.