9709/43

Mathematics 9709/43October/November 2010

Cambridge A-Level · Mechanics · worked solutions for every part, with the mark scheme

7
questions
50
marks
75
minutes

Topics Kinematics of Motion in a Straight Line · Newton's Laws of Motion · Energy, Work and Power · Forces and Equilibrium

Q14MNewton's Laws of MotionKinematics of Motion in a Straight LineFree sample

A particle PP is released from rest at a point on a smooth plane inclined at 3030^{\circ} to the horizontal. Find the speed of PP

(i) when it has travelled 0.9 m0.9\text{ m},
(ii) 0.8 s0.8\text{ s} after it is released.

DifficultyMedium-Easy
Worked solution

Approach

The plane is smooth, so there is no friction. The only force with a component along the plane is the weight mgmg. Resolving parallel to the plane:

ma=mgsin30ma = mg\sin 30^\circ

so

a=gsin30=10×12=5 m s2.a = g\sin 30^\circ = 10 \times \frac12 = 5\ \text{m s}^{-2}.

Then apply the constant-acceleration (suvat) equations with u=0u = 0.

Working

Part (i): distance travelled s=0.9 ms = 0.9\ \text{m}

Use v2=u2+2asv^2 = u^2 + 2as:

v2=02+2(5)(0.9)=9v^2 = 0^2 + 2(5)(0.9) = 9 v=3 m s1.v = 3\ \text{m s}^{-1}.

Part (ii): time elapsed t=0.8 st = 0.8\ \text{s}

Use v=u+atv = u + at:

v=0+5(0.8)=4 m s1.v = 0 + 5(0.8) = 4\ \text{m s}^{-1}.

Answer

(i) Speed is 3 m s13\ \text{m s}^{-1}; (ii) Speed is 4 m s14\ \text{m s}^{-1}.

Final answer

Part (i): 3 m s^-1; Part (ii): 4 m s^-1

Detailed explanation

Walkthrough

The particle is released from rest on a smooth plane inclined at 3030^\circ to the horizontal. Because the plane is smooth, there is no friction, so the only forces acting are the weight mgmg vertically downwards and the normal reaction force RR perpendicular to the plane.

The normal reaction has no component down the plane. The weight does have a component mgsin30mg\sin 30^\circ down the plane. Applying Newton's second law parallel to the plane:

ma=mgsin30ma = mg\sin 30^\circ

so the mass cancels, and

a=gsin30=5 m s2.a = g\sin 30^\circ = 5\ \text{m s}^{-2}.

This acceleration is constant, so we can use the suvat equations for motion in a straight line. In both parts the initial velocity is u=0u=0.

For part (i), we know uu, aa and s=0.9s=0.9 and want vv; the equation linking these is v2=u2+2asv^2=u^2+2as. Substituting gives v2=9v^2=9, so v=3 m s1v=3\ \text{m s}^{-1}.

For part (ii), we know uu, aa and t=0.8t=0.8 and want vv; the equation linking these is v=u+atv=u+at. Substituting gives v=4 m s1v=4\ \text{m s}^{-1}.

An equivalent energy approach for part (i) would be to equate the loss in gravitational potential energy mg(0.9sin30)mg(0.9\sin30^\circ) to the gain in kinetic energy 12mv2\frac12 mv^2; the mass cancels and gives the same result.

Key Takeaways

  • On a smooth inclined plane the acceleration down the plane is gsinθg\sin\theta, and it does not depend on the mass of the particle.
  • The component of weight along a plane inclined at angle θ\theta is mgsinθmg\sin\theta.
  • Choose the suvat equation that contains the three known quantities and the required unknown.
  • Smooth contact means no friction, so only the gravitational component causes acceleration along the plane.

Common Mistakes

  • Including a frictional force on a smooth plane. A smooth plane means friction is zero.
  • Using the whole weight mgmg instead of the component mgsin30mg\sin30^\circ along the plane.
  • Trying to use v=u+atv=u+at in part (i), where the distance is given but the time is not directly known.
  • Forgetting to take the positive square root when using v2=u2+2asv^2 = u^2 + 2as.
  • Forgetting units or writing the answers without m s1\text{m s}^{-1}.

Things to Be Careful About

  • Use g=10 m s2g = 10\ \text{m s}^{-2} unless the question states another value.
  • Keep all quantities in metres and seconds; displacement 0.90.9 m and time 0.80.8 s are already in consistent units.
  • The acceleration is down the plane; take this direction as positive, so the speed is positive.
  • If using the energy method, remember the vertical height lost is ssin30s\sin30^\circ, not the distance along the plane.
Techniques used
resolve the weight into components parallel to the planeapply Newton's second law to determine the accelerationapply the suvat equation linking displacement and velocityapply the suvat equation linking time and velocity

The rest of this paper

6 more questions
  • Q2Energy, Work and Power4M
  • Q3Forces and Equilibrium7M
  • Q4Kinematics of Motion in a Straight Line7M
  • Q5Forces and Equilibrium7M
  • Q6Kinematics of Motion in a Straight Line8M
  • Q7Energy, Work and Power · Newton's Laws of Motion13M
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