Accelaration due to Gravity
Purpose of the lab report: to report what you did, what you observed, and what it means.
Section Purpose
Abstract Answers the question: “What is a summary of what you did and what you found out?” (Write this last!)
Introduction Answers the question: “What was the motivation for this experiment and what broad strategy did you use?”
Methods Answers the question: “What exactly did you do?”
Experimental Setup
Describe your experimental set up, including each component and how you used it.
Precautions What lab precautions should be taken for this specific lab.
Data Answers the question: “What did you observe?”
Analysis Answers the question: “What do your observations mean?”
Assess Did you get results you expected from your understanding of theory and concepts? Did you get results that match standard values? Discuss what may have contributed to any deviation from standard values. Even if there were no deviation from standard values, explain what careful steps you took to get this result. This is a very important part of any experiment.
Sample Formal Laboratory Report with some of the information mentioned above
Checking the Speedometer of a Car
Alex Wong
9/25/2012
Abstract: The accuracy of a speedometer reading in a 1997 Toyota corolla was tested by
measuring the time it took the corolla to travel a range of distances (0-200m) when driven at a
constant speed of 100km/hr, as measured using the speedometer. The experimental speed
measurements were consistent with the speedometer reading. However, uncertainty in the
experiment was ±10.1%, so speedometer inaccuracies of 10% or less cannot be ruled out.
Introduction: I am often unsure of how reliable my speedometer is, so verifying its accuracy
could help me avoid costly tickets. We tested the accuracy of the speedometer in a 1997 Toyota
corolla by driving the corolla at a constant speed down a straight road and measuring the time it
took for the corolla to cover a range of distances.
Methods: A long straight stretch of road was identified near Largo MD. A traffic cone was
placed along the side of the road. A tape measure was used to measure distances 50m, 100m,
150m, and 200m along the road away from the cone, and cones were placed at each of these four
locations (Figure 1). Five stopwatches were coordinated to the nearest 1/100th of a second. Five
observers each took one of these watches and stood by each of the cones. A driver in the corolla
then drove the car along the stretch of road, maintaining a constant speed of 100km/hr according
to the speedometer. Each of the five observers noted the time when the car passed him or her.
Figure 1.
Data: The times recorded by each observer are reported in the table below:
Observer Location (±0.1m) Time (±0.25s)
Alex 0m 11:59:12.59
Beth 50m 11:59:14.67
Charlie 100m 11:59:16.05
Diana 150m 11:59:17.86
Ester 200m 11:59:19.85
The main factor causing uncertainty in the location measurements was the difficulty in stretching
the tape measure perfectly straight. The main factor causing uncertainty in the time
measurements were possibly varying reaction times of the observers.
The driver observed that the speedometer did not vary more than 2km/hr from 100km/hr during
the time in which she drove the car. Therefore the uncertainty in the speedometer reading was
±2km/hr.
Analysis:
In order to simplify our analysis we first define time t=0 to be the time the car passed the cone at
x=0m. Our time data was then expressed as the amount of time elapsed after the car passed the
first cone:
Observer Location (±0.1%) Time (±8%)
Alex 0m 0
Beth 50m 2.08
Charlie 100m 3.46
Diana 150m 5.27
Ester 200m 7.26
Percent uncertainty in the location is (±0.1m/100m)*100=0.1%. Percent uncertainty in the time
is (±0.25s/3.6s)*100=8%.
Since for an object moving with constant velocity x=x0+v*t, we expect that if we plot the
position vs. the time we will get a linear graph, and the slope of that graph will be the velocity of
the car. Figure 2 shows this graph.
Figure 2.
A linear regression of the data has an r2 value of 0.9965 indicating that the data is in fact quite
linear, confirming that the far was travelling at close to a constant velocity.
Using the regression equation we are able to find the explicit function for the position as a
function of time:
x = 28.1(m/s)*t - 1.68m
The slope of the regression line, 28.1m/s, is the experimental estimate for the speed of the car.
Since the uncertainty in the position is ±0.1% and the uncertainty in the time is ±8%, the
uncertainty in our experimental estimate for the velocity is 8 + 0.1 =8.1%, so our experimental
velocity is 28.1m/s ± 8.1%.
Our theoretical velocity, according to the speedometer, is 100km/hr ± 2km/hr = 100km/hr ± 2%
= 27.8m/s ± 2%.
The discrepancy between the speedometer measurement and the experimental measurement is
0.3m/s, or 100 * (0.3/27.8) = 1%. Our total uncertainty is 8.1% + 2% = 10.1%. Since the
discrepancy is less than the uncertainty, or experimental measurement of the speed of the car is
consistent with the speedometer value. However, this does not prove that the speedometer value
is accurate: our experimental design was expected to be accurate to only ±10.1%. Therefore, our
experiment could have detected speedometer errors of only 10.1% or greater. It is still possible
that the speedometer is inaccurate, but our experiment has shown that the speedometer is not
inaccurate by more than about 10%.
References:
1. Fredrick, Hans. “The accuracy of Vehicle Speedometers”.
http://www.ehow.com/info_12209329_accuracy-vehicle-speedometers.html. Accessed
9/25/2012.
y = 28.135x - 1.679 R² = 0.9965
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