Lab 3 Uniformly accelerated motion

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Arizona State University *

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Dec 6, 2023

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Lab 3: Uniformly Accelerated Motion 1. Testable Question: How does the instantaneous velocity relate to the distance of the car? 2. Hypothesis: If the distance traveled increases, then the velocity will also increase because this allows gravity to pull the car closer to the ground. 3. Variables: Control(s): track angle ( ), mass of cart/fence (m), Initial position, Velocity (x 0 , v 0 ) Independent: Distance (X) Dependent: Velocity (V) 4. Experimental Design: m, x 0 , v 0 i ( o ) X(m) V (m/s) 1–8 1 X 1-8 V 1-8 1–8 2 X 1-8 V 1-8 5. Materials: Cart Track Picket fence 1 photogate Ring stand 4 bumpers Spark XLi 6. Procedure: Setup:
1. Set up station as shown in the diagram above 2. Place car 0.1 m away from the sensor 3. Release the car and record data provided by the photogate and Spark XLi 4. Repeat adding 0.100 m per measurement until you reach the distance of 0.800 m 5. v 2 = v 0 2 +2a x Example: To get a near instantaneous speed of an object: Use one photogate. Measure and attach the smallest, single black rectangle (flag) on a picket fence See top flag in the figure below. This will block the light beam when it enters the gate. Make sure the photogate is set at the correct height for this black rectangle. Set the gate to collect the “ Time in Gate ” or “ Velocity in Gate ,” depending on the desired data output. For the latter, the width of the flag must be entered into the SPARK LXi. If just the timing data is collected, the speed can be calculated using the average speed in the gate:
average speed , ´ v = flag ¿ ∆x time gate,∆t ∨´ v = ∆ x ∆t The angle of the track will be measured two ways. First, there is a free app called Angle Pro that can measure an angle to 0.1°. Second, using trigonometry, measure the length of the track (around 122.0cm) and its height above a suitable reference point. Then use the inverse sine to get the angle ( do not use angles greater than 15 ° ) : Low Angle θ = sin 1 ( 9.9 122.0 cm ) ¿ 4.65 0 High Angle θ = sin 1 ( 18 122.0 cm ) ¿ 8.48 0 The acceleration on the track, a , can be calculated using the accepted value for the acceleration due to gravity, g , and the sine of the angle of the track: a = g ∙sin θ = g ∆ y 122.0 cm Two runs of the experiment will be conducted. The last step in the procedures should present the equation that is being investigated in the lab. Consult the Physics Equations resource. 7. Data: =4.65 =5.65 i x (m) x1/2(m1/2 ) v (m/s) v (m/s) 1 0.1 0.316 0.522 0.576 2 0.2 0.447 0.554 0.772 3 0.3 0.548 0.669 0.955
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4 0.4 0.632 0.780 1.090 5 0.5 0.707 0.776 1.221 6 0.6 0.775 0.859 1.334 7 0.7 0.837 0.942 1.436 8 0.8 0.894 1.011 1.543 m=260g Controls x0= 0m v0= 0m/s 8. Analysis: 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 0.000 0.200 0.400 0.600 0.800 1.000 1.200 1.400 1.600 1.800 Velocity vs Distnace Low Angle High Angle Distance (m) Velocity (m/s) 0.200 0.300 0.400 0.500 0.600 0.700 0.800 0.900 1.000 0.000 0.200 0.400 0.600 0.800 1.000 1.200 1.400 1.600 1.800 f(x) = 1.73 x R² = 1 f(x) = 1.16 x R² = 0.99 v vs x1/2 v (m/s) Linear (v (m/s)) v (m/s) Linear (v (m/s)) x1/2(m1/2) V (m/s)
Low Angle 4.65 TS= 2 a TS = 2 9.81 m / s 2 sin 4.65 =.75 m s MS = 1.16 m s % error = | 0.75 1.16 | 0.75 × 100 ¿ | 0.41 | 1.7 × 100 = 54.7 % High Angle 8.48 TS = 2 a TS = 2 9.81 m / s 2 sin 8.48 = 1.7 m s
MS = 1.73 m s % error = | 1.7 1.73 | 1.7 × 100 = | . 03 | 1.7 × 100 = 1.76% 9. Conclusion: Velocity is directly proportional to square root of the cars position, according to: Low Angle: v= (1.16m ½) x 1/2 High Angle: v= (1.73m ½) x ½ As the initial distance of the car from the sensor increased, the velocity also increased. This increase was due to the car having a longer time to travel resulting in faster speed from the influence of gravity. As the ramp angle increased, the acceleration and velocity showed a direct increase. 10. Evaluation: During this experiment, velocity and distance showed a direct proportion as when the distance increased so did the velocity. Results regarding the accuracy showed a high error percent. The percent error associated with the low angle reflected a 54.7%. This is considered to be an extremely high percent error. The TS of the low angle was 0.75 m s and the MS of the low angle resulted in 1.16 m s . When looking at the high angle, the percent error reflected a 1.76%, which is a low percent error. Reasons for the percent error resulting in an extremely high score could be a result of systematic errors which could include the Spark XLi being moved by a peer or the car being released at a further distance resulting in inaccuracy throughout measurements. The R2 value collected from the low angle reflected a 0.9931 and the high angle
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reflecting a 0.9999. These values represent an outstanding precision score. Though minor random errors can occur such as releasing the car with additional force.