Experiment 2: Uniformly Accelerated Motion — Worked Examples

The following examples connect stopwatch-and-distance measurements with the graphs used to verify approximately constant acceleration.

Example 1: Acceleration from one distance-time measurement

A trolley is released from rest and travels 0.800 m0.800\,\text{m} in 1.60 s1.60\,\text{s}. Assuming constant acceleration, determine aa.

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Example 2: Acceleration from a d-versus-t² graph

A best-fit line of distance dd versus t2t^2 has slope 0.318 m/s20.318\,\text{m/s}^2. Determine the trolley acceleration.

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Example 3: Average velocity over a measured interval

The trolley position changes from 0.30 m0.30\,\text{m} at 0.95 s0.95\,\text{s} to 0.62 m0.62\,\text{m} at 1.35 s1.35\,\text{s}. Determine the average velocity.

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Example 4: Instantaneous velocity predicted from constant acceleration

Using a=0.636 m/s2a=0.636\,\text{m/s}^2 and release from rest, determine the instantaneous velocity at t=1.50 st=1.50\,\text{s}.

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Example 5: Acceleration from a velocity-time graph

A best-fit velocity-time line passes through (0.40 s,0.23 m/s)(0.40\,\text{s},0.23\,\text{m/s}) and (1.60 s,0.98 m/s)(1.60\,\text{s},0.98\,\text{m/s}). Determine the acceleration.

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Example 6: Ideal incline prediction versus measured acceleration

A rail is inclined at 4.0∘4.0^\circ. Neglecting rolling resistance, predict the along-track acceleration gsin⁡θg\sin\theta. If the measured value is 0.625 m/s20.625\,\text{m/s}^2, determine the shortfall relative to the ideal prediction. Use g=9.80665 m/s2g=9.80665\,\text{m/s}^2.

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Example 7: Detecting a nonzero release velocity

A linear fit of dd versus t2t^2 gives a nonzero intercept, while a fit of dd versus tt over the earliest measurements suggests the trolley already had forward velocity at release. Explain how the governing equation changes.

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Example 8: Timing error sensitivity

For fixed distance, a=2d/t2a=2d/t^2. A true travel time is 1.60 s1.60\,\text{s}, but a reaction-time delay produces a recorded value of 1.62 s1.62\,\text{s}. Determine the ratio of the calculated acceleration to the true acceleration.

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