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Questions on motion graphs and the SUVAT equations
Gradient and area read every motion graph: gradient gives velocity on a displacement-time graph and acceleration on a velocity-time graph. The area beneath a velocity-time graph is the displacement, whatever shape the curve takes. The four SUVAT equations are quicker but hold only while the acceleration stays constant.
21 original questions · 72 marks · the motion graphs and the SUVAT equations notes · Mechanics
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Jump to: Reading the motion graphs · The constant-acceleration equations
Reading the motion graphs
Distinguish between the average velocity and the instantaneous velocity of a moving object.
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Average velocity is total displacement divided by total time (1). Instantaneous velocity is the rate of change of displacement at one instant, that is the gradient of the displacement–time graph at that point (1).State what the gradient and the area under a velocity–time graph each represent.
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The gradient represents acceleration (1); the area between the line and the time axis represents displacement (1).On a displacement–time graph, state what is represented by (a) the gradient at a point, and (b) a horizontal section of the line.
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(a) The instantaneous velocity at that point (1). (b) The object is stationary; its displacement is not changing (1).An object accelerates uniformly from rest to 15 m s−1 in 5.0 s, then travels at a constant 15 m s−1 for a further 10 s. Using the area under the velocity–time graph, calculate the total distance travelled.
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Distance = ½ × 5.0 × 15 (area of the triangle) (1)
+ 15 × 10 (area of the rectangle) (1)
Distance = 188 m (1)The velocity–time graph of a journey is a straight line sloping upwards from a non-zero starting velocity. Explain how you would find the acceleration and the displacement from this graph.
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The acceleration is the gradient of the line, change in velocity divided by change in time (1). The displacement is the area of the trapezium between the line and the time axis (1), which equals ½(u + v)t (1).A ball is released from rest, falls to a hard floor and bounces repeatedly, each bounce reaching a smaller height than the last, until it comes to rest. Air resistance is negligible while the ball is in flight. Taking downward velocity as positive, describe fully the velocity–time graph of the motion from release until the ball stops bouncing.
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During every flight the graph is a straight line of gradient +g (9.81 m s−2), because gravity is the only force acting (1). Every up and every down section has this same gradient (1). From release the velocity rises from zero to its largest positive value just before the first impact (1). At each bounce the line is almost vertical: the velocity reverses from positive (downwards) to negative (upwards) in a very short contact time (1). Each rebound speed is smaller than the impact speed before it, because energy is lost in the bounce, so the peaks of the graph shrink (1). The velocity passes through zero at the top of each bounce, and the graph ends at v = 0 when the ball comes to rest (1).A car moves along a straight road for 20 s. Motion in one direction is taken as positive. Determine the displacement of the car from its starting point at the end of the 20 s, and the total distance it has travelled.
The car's velocity over the whole 20 s. The line changes slope twice and crosses the time axis once, and every value this question needs is read from the axes. Mark scheme
Displacement is the area between the line and the time axis, and area below the axis counts as negative because the car has reversed (1)
Above the axis the area is ½ × 6.0 × 12 + 6.0 × 12 + ½ × 6.0 × 12 = 36 + 72 + 36 = 144 m (1)
The line crosses the axis at t = 18 s, so the area below it is ½ × 2.0 × 4.0 = 4.0 m, and the displacement is 144 − 4.0 = 140 m (1)
Distance takes no account of direction, so the last 4.0 m is added rather than subtracted, giving 148 m (1)
The constant-acceleration equations
A car starts from rest and accelerates uniformly at 2.0 m s−2 for 6.0 s. Calculate its final velocity.
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v = u + at = 0 + 2.0 × 6.0 (1)
v = 12 m s−1 (1)A tram slows uniformly from 12.0 m s−1 to 3.0 m s−1 in 6.0 s. Calculate its acceleration.
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a = Δv/Δt = (3.0 − 12.0)/6.0 (1) = −1.5 m s−2, a deceleration of 1.5 m s−2 (1).State the condition that must be satisfied for the SUVAT equations to be valid.
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The acceleration must be constant (uniform) throughout the motion (1).A car travelling at 8.0 m s−1 accelerates uniformly at 1.5 m s−2 for 4.0 s. Calculate (a) its final velocity and (b) the distance travelled in this time.
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(a) v = u + at = 8.0 + 1.5 × 4.0 (1)
v = 14 m s−1 (1)
(b) s = ut + ½at2 = 8.0 × 4.0 + ½ × 1.5 × 4.02 (1)
s = 44 m (1)A car travelling at 20 m s−1 brakes uniformly and stops in a distance of 40 m. Calculate (a) its deceleration and (b) the time taken to stop.
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(a) v2 = u2 + 2as gives a = −(202)/(2 × 40) (1)
a = −5.0 m s−2, a deceleration of 5.0 m s−2 (1)
(b) t = v/|a| = 20/5 (1)
t = 4.0 s (1)A stone is dropped from rest and falls freely. Taking g = 9.81 m s−2, calculate its velocity and the distance fallen after 2.0 s.
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v = gt = 9.81 × 2.0 = 19.6 m s−1 (1)
s = ½gt2 = ½ × 9.81 × 2.02 (1)
s = 19.6 m (1)A student measures a friend's reaction time by dropping a ruler between the friend's open fingers. The friend catches the ruler after it has fallen 28 cm from rest. Taking g = 9.81 m s−2, show that the reaction time is about 0.24 s.
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From rest, s = ½gt2, so t = √(2s/g) (1). t = √(2 × 0.28/9.81) (28 cm converted to 0.28 m) (1) = 0.239 s ≈ 0.24 s (1).A skateboarder is moving at 1.2 m s−1 at the top of a ramp. She accelerates uniformly down the ramp at 2.5 m s−2 over a distance of 4.2 m. Calculate her speed at the bottom of the ramp.
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v2 = u2 + 2as (1) = 1.22 + 2 × 2.5 × 4.2 = 22.4 (1), so v = 4.7 m s−1 (1).A goods train travels at 90 km h−1. The driver applies the brakes and the train decelerates uniformly at 0.75 m s−2. Calculate the minimum distance the train travels before stopping.
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u = 90 km h−1 = 90 000/3600 = 25 m s−1 (1). With v = 0: v2 = u2 + 2as (1), so s = 252/(2 × 0.75) (1) = 417 m ≈ 420 m (1).A train starts from rest and accelerates uniformly at 0.50 m s−2 for 20 s. The driver then brakes and the train decelerates uniformly to rest in a further 100 m. Calculate (a) the maximum velocity of the train, (b) the deceleration while braking, and (c) the total distance travelled.
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(a) v = u + at = 0 + 0.50 × 20 = 10 m s−1 (1)
(b) v2 = u2 + 2as gives a = −102/(2 × 100) (1)
a = −0.50 m s−2, a deceleration of 0.50 m s−2 (1)
(c) Accelerating: s = ½at2 = ½ × 0.50 × 202 = 100 m (1)
Total = 100 + 100 = 200 m (1)A ball is thrown vertically upwards at 15 m s−1. Taking g = 9.81 m s−2 and ignoring air resistance, calculate (a) the maximum height reached and (b) the time taken to reach it.
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(a) At the top v = 0, so h = u2/2g = 152/(2 × 9.81) (1)
h = 11.5 m (1)
(b) t = u/g = 15/9.81 (1)
t = 1.53 s (1)A delivery van passes a stationary motorcycle courier, travelling at a constant 16 m s−1 along a straight road. At the instant it passes, the courier sets off after it with a uniform acceleration of 2.0 m s−2. (a) Show that the courier draws level with the van 16 s after setting off. (b) Go on to calculate the distance travelled and the courier's speed at that moment.
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(a) Equal displacements when the courier draws level: 16t = ½ × 2.0 × t2 (1), so t = 16 s (1). (b) s = 16 × 16 = 256 m (1). v = u + at = 2.0 × 16 (1) = 32 m s−1 (1).A car travels at 20 m s−1 towards a pelican crossing. When the car is 42 m from the stop line, the lights change and the driver decides to stop. The driver's reaction time is 0.60 s and the car's maximum deceleration is 5.0 m s−2. Deduce whether the car can stop before the stop line.
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Thinking distance = 20 × 0.60 = 12 m (1). Braking distance = v2/2a = 202/(2 × 5.0) = 40 m (1). Stopping distance = 12 + 40 = 52 m (1). 52 m is greater than 42 m, so the car cannot stop before the line (1).Derive the four constant-acceleration equations from the definition of acceleration and the definition of average velocity. State which step of your derivation uses the condition that the acceleration is constant.
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With a constant acceleration the average and the instantaneous rate of change of velocity are the same, so a = (v − u)/t, which rearranges to v = u + at (1). Displacement is average velocity × time, and under a constant acceleration the average velocity is the mean of the end values, ½(u + v), giving s = ½(u + v)t (1). Substituting the first result into the second: s = ½(u + u + at)t = ½(2u + at)t (1), which multiplies out to s = ut + ½at2 (1). Eliminating t instead: t = (v − u)/a, so s = ½(u + v)(v − u)/a, and multiplying both sides by 2a gives 2as = (v + u)(v − u) = v2 − u2, that is v2 = u2 + 2as (1). The condition is used in the second step, where the average velocity is taken as the mean of the first and last values; that is false as soon as the acceleration varies (1).
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