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9231 · 3.5

Linear motion under a variable force — practice questions

Practice and worked examples for 9231 Linear motion under a variable force. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

A particle P of mass 0.5 kg moves in a straight line. At time tt seconds, the net force acting on P is (2t+1)(2t+1) N. When t=0t=0, the particle is at rest at the origin O. Find the velocity and displacement of P from O when t=4t=4 s.

Show solution outline

The force is a function of time, F(t)=2t+1F(t) = 2t+1. We use Newton's Second Law, F=maF=ma.

2t+1=0.5a2t+1 = 0.5a

Since force is a function of time, we use a=dvdta = \frac{dv}{dt}.

2t+1=0.5dvdt2t+1 = 0.5 \frac{dv}{dt}

4t+2=dvdt4t+2 = \frac{dv}{dt}

To find vv, we integrate with respect to tt:

v=(4t+2)dt=2t2+2t+Cv = \int (4t+2) \,dt = 2t^2 + 2t + C

We are given that P is at rest when t=0t=0, so v=0v=0 when t=0t=0. 0=2(0)2+2(0)+C    C=00 = 2(0)^2 + 2(0) + C \implies C=0.

So, the velocity at time tt is v=2t2+2tv = 2t^2 + 2t.

When t=4t=4 s: v=2(4)2+2(4)=2(16)+8=32+8=40v = 2(4)^2 + 2(4) = 2(16) + 8 = 32 + 8 = 40 m/s.

To find displacement xx, we use v=dxdtv = \frac{dx}{dt}.

dxdt=2t2+2t\frac{dx}{dt} = 2t^2 + 2t

Integrate with respect to tt:

x=(2t2+2t)dt=23t3+t2+Dx = \int (2t^2 + 2t) \,dt = \frac{2}{3}t^3 + t^2 + D

We are given that P is at the origin when t=0t=0, so x=0x=0 when t=0t=0. 0=23(0)3+(0)2+D    D=00 = \frac{2}{3}(0)^3 + (0)^2 + D \implies D=0.

So, the displacement at time tt is x=23t3+t2x = \frac{2}{3}t^3 + t^2.

When t=4t=4 s: x=23(4)3+(4)2=23(64)+16=1283+483=176358.7x = \frac{2}{3}(4)^3 + (4)^2 = \frac{2}{3}(64) + 16 = \frac{128}{3} + \frac{48}{3} = \frac{176}{3} \approx 58.7 m (3 s.f.).

Answer: At t=4t=4 s, velocity is 40 m/s and displacement is 1763\frac{176}{3} m.

Worked example 2

A particle of mass 2 kg is acted on by a force of magnitude 18x2\frac{18}{x^2} N, directed away from the origin O. The particle is projected from the point x=3x=3 with a velocity of 4 m/s towards O. Find its speed when it reaches the point x=6x=6.

Show solution outline

The force is a function of displacement, F(x)=18x2F(x) = \frac{18}{x^2}. The force is directed away from O, so it's in the positive xx direction.

Using Newton's Second Law, F=maF=ma:

18x2=2a\frac{18}{x^2} = 2a

Since force is a function of xx, we use a=vdvdxa = v\frac{dv}{dx}.

18x2=2vdvdx\frac{18}{x^2} = 2v\frac{dv}{dx}

9x2=vdvdx\frac{9}{x^2} = v\frac{dv}{dx}

Now, we separate the variables:

9x2dx=vdv\int \frac{9}{x^2} \,dx = \int v \,dv

Integrating both sides:

9x+C=12v2-\frac{9}{x} + C = \frac{1}{2}v^2

We are given the initial conditions: at x=3x=3, the velocity is 44 m/s towards O. Since the positive direction is away from O, the velocity is v=4v = -4 m/s.

Substitute these values to find C:

93+C=12(4)2-\frac{9}{3} + C = \frac{1}{2}(-4)^2

3+C=12(16)=8-3 + C = \frac{1}{2}(16) = 8

C=11C = 11

So the relationship between vv and xx is: 12v2=119x\frac{1}{2}v^2 = 11 - \frac{9}{x}.

We need to find the speed when x=6x=6. Speed is the magnitude of velocity. Let's find v2v^2.

At x=6x=6:

12v2=1196=111.5=9.5\frac{1}{2}v^2 = 11 - \frac{9}{6} = 11 - 1.5 = 9.5

v2=19v^2 = 19

v=±19v = \pm\sqrt{19}

The speed is the magnitude of the velocity, which is v|v|.

Speed = 194.36\sqrt{19} \approx 4.36 m/s (3 s.f.).

Answer: The speed of the particle at x=6x=6 is 19\sqrt{19} m/s.