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9709 · 4.2

Kinematics of motion in a straight line — practice questions

Practice and worked examples for 9709 Kinematics of motion in a straight line. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

A car is travelling along a straight road at 12 m s⁻¹. It accelerates uniformly at 1.5 m s⁻² for 8 seconds. Find the car's final velocity and the distance it travels during this time.

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First, list the known SUVAT variables. We are given: u=12 m s1u = 12 \text{ m s}^{-1} a=1.5 m s2a = 1.5 \text{ m s}^{-2} t=8 st = 8 \text{ s}

We need to find the final velocity, vv, and the displacement, ss.

To find v: Choose the equation that links u, a, t, and v: v=u+atv = u + at. v=12+(1.5)(8)v = 12 + (1.5)(8) v=12+12v = 12 + 12 v=24 m s1v = 24 \text{ m s}^{-1}

To find s: We can use an equation linking u, a, t, and s: s=ut+12at2s = ut + \frac{1}{2}at^2. s=(12)(8)+12(1.5)(82)s = (12)(8) + \frac{1}{2}(1.5)(8^2) s=96+12(1.5)(64)s = 96 + \frac{1}{2}(1.5)(64) s=96+48s = 96 + 48 s=144 ms = 144 \text{ m}

The final velocity is 24 m s⁻¹ and the distance travelled is 144 m.

Worked example 2

The velocity-time graph for a cyclist's journey is a straight line from (0, 4) to (10, 12), where time is in seconds and velocity is in m s⁻¹. Calculate the acceleration of the cyclist and the total distance travelled in the 10 seconds.

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The graph is a straight line, which means the acceleration is constant.

To find acceleration, a: Acceleration is the gradient of the v-t graph. a=change in velocitychange in time=v2v1t2t1a = \frac{\text{change in velocity}}{\text{change in time}} = \frac{v_2 - v_1}{t_2 - t_1} a=124100=810a = \frac{12 - 4}{10 - 0} = \frac{8}{10} a=0.8 m s2a = 0.8 \text{ m s}^{-2}

To find distance travelled, s: Distance travelled is the area under the v-t graph. The shape is a trapezium. Area = 12(a+b)h\frac{1}{2}(a+b)h, where a and b are the parallel sides (the initial and final velocities) and h is the height (the time interval). s=12(4+12)×10s = \frac{1}{2}(4 + 12) \times 10 s=12(16)×10s = \frac{1}{2}(16) \times 10 s=8×10=80 ms = 8 \times 10 = 80 \text{ m}

The cyclist's acceleration is 0.8 m s⁻² and the total distance travelled is 80 m.

Worked example 3

A particle moves in a straight line. Its acceleration at time tt seconds is given by a=(6t2)a = (6t - 2) m s⁻². When t=0t=0, the particle is at the origin and has a velocity of 3 m s⁻¹. Find expressions for its velocity and displacement in terms of tt.

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We are given a=6t2a = 6t - 2.

To find velocity, v: Integrate acceleration with respect to time. v=adt=(6t2)dtv = \int a \, dt = \int (6t - 2) \, dt v=3t22t+Cv = 3t^2 - 2t + C We are given that when t=0t=0, v=3v=3. Substitute these values to find C: 3=3(0)22(0)+C    C=33 = 3(0)^2 - 2(0) + C \implies C = 3 So, the expression for velocity is v=3t22t+3v = 3t^2 - 2t + 3 m s⁻¹.

To find displacement, s: Integrate velocity with respect to time. s=vdt=(3t22t+3)dts = \int v \, dt = \int (3t^2 - 2t + 3) \, dt s=t3t2+3t+Ds = t^3 - t^2 + 3t + D We are given that when t=0t=0, the particle is at the origin, so s=0s=0. Substitute these values to find D: 0=(0)3(0)2+3(0)+D    D=00 = (0)^3 - (0)^2 + 3(0) + D \implies D = 0 So, the expression for displacement is s=t3t2+3ts = t^3 - t^2 + 3t m.