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Momentum and impulse in vector formEdexcel International A Level Further Maths: Revision notes

Section 1

Momentum as a vector

The momentum of a particle of mass mm and velocity v\mathbf{v} is mvm\mathbf{v}, a vector in the same direction as the velocity, measured in kg m s−1^{-1} (or N s). Mass is a scalar, so multiplying scales each component: a 22 kg particle with velocity 4i−j4\mathbf{i}-\mathbf{j} has momentum 8i−2j8\mathbf{i}-2\mathbf{j}. The speed is the magnitude of the velocity, vx2+vy2\sqrt{v_x^2+v_y^2}, and the direction is found with tan⁡θ=vyvx\tan\theta=\frac{v_y}{v_x} (check the quadrant). Momentum and velocity are vectors, so they add as vectors; speeds do not.

Key termsmomentumvectorspeed
Common mistake

Adding speeds instead of vectors. Always work with i\mathbf{i} and j\mathbf{j} components separately.

Section 2

Impulse and the impulse-momentum principle

The impulse of a constant force F\mathbf{F} acting for a time tt is I=Ft\mathbf{I}=\mathbf{F}t, measured in N s. The impulse-momentum principle says that the impulse equals the change in momentum: I=mv−mu=m(v−u).\mathbf{I}=m\mathbf{v}-m\mathbf{u}=m(\mathbf{v}-\mathbf{u}). In vector form this applies to each component separately. Example: a 0.40.4 kg ball changes velocity from 6i+8j6\mathbf{i}+8\mathbf{j} to −2i+5j-2\mathbf{i}+5\mathbf{j}: I=0.4(−8i−3j)=−3.2i−1.2j\mathbf{I}=0.4(-8\mathbf{i}-3\mathbf{j})=-3.2\mathbf{i}-1.2\mathbf{j} N s. If the impulse is given, rearrange: v=u+Im\mathbf{v}=\mathbf{u}+\frac{\mathbf{I}}{m}.

Key termsimpulseimpulse-momentum principle
Common mistake

Writing m(u−v)m(\mathbf{u}-\mathbf{v}). Impulse is final minus initial, and it is in the direction of the force applied.

Section 3

Magnitude and direction of an impulse

The magnitude of I=ai+bj\mathbf{I}=a\mathbf{i}+b\mathbf{j} is a2+b2\sqrt{a^2+b^2} and its direction is the direction of the force that acted on the particle. For −3.2i−1.2j-3.2\mathbf{i}-1.2\mathbf{j} the magnitude is 11.68=3.42\sqrt{11.68}=3.42 N s, at tan⁡−11.23.2=20.6∘\tan^{-1}\frac{1.2}{3.2}=20.6^\circ below the direction of −i-\mathbf{i}. To find the angle through which a particle is turned, find the direction of u\mathbf{u} and of v\mathbf{v} (each from tan⁡−1\tan^{-1}, checking the quadrant) and subtract, or use the scalar product.

Key termsmagnitude
Exam tip

Sketch the vector first, so you can see which quadrant the angle is in.

Section 4

Conservation of linear momentum

When two particles collide and there is no external impulse (for example on a smooth horizontal plane), the total momentum is unchanged: m1u1+m2u2=m1v1+m2v2.m_1\mathbf{u}_1+m_2\mathbf{u}_2=m_1\mathbf{v}_1+m_2\mathbf{v}_2. This vector equation gives two scalar equations, one for i\mathbf{i} and one for j\mathbf{j}. If the particles coalesce they move together, so m1u1+m2u2=(m1+m2)vm_1\mathbf{u}_1+m_2\mathbf{u}_2=(m_1+m_2)\mathbf{v}. Newton's third law means the impulse on each particle is equal in size and opposite in direction, which is why total momentum is conserved.

Key termsconservation of linear momentumcoalesce
Exam tip

Keep a table: mass, velocity before, velocity after, for each particle, in vector form.

Section 5

Worked example and method

AA (22 kg) has velocity 4i−j4\mathbf{i}-\mathbf{j} and BB (33 kg) has velocity −2i+3j-2\mathbf{i}+3\mathbf{j}. After the collision AA has velocity −i+2j-\mathbf{i}+2\mathbf{j}. Total momentum: 2(4i−j)+3(−2i+3j)=2i+7j2(4\mathbf{i}-\mathbf{j})+3(-2\mathbf{i}+3\mathbf{j})=2\mathbf{i}+7\mathbf{j}. So 2i+7j=2(−i+2j)+3vB2\mathbf{i}+7\mathbf{j}=2(-\mathbf{i}+2\mathbf{j})+3\mathbf{v}_B, giving vB=43i+j\mathbf{v}_B=\frac43\mathbf{i}+\mathbf{j} and speed 53\frac53 m s−1^{-1}. Method: (1) write each momentum as a vector; (2) apply the principle; (3) solve component by component; (4) find magnitudes and angles last. The impulse on one particle is m(v−u)m(\mathbf{v}-\mathbf{u}); on the other it is minus that.

Exam tip

Check by working out the impulse on both particles: they must be equal and opposite.

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Carry on to the next subtopic.

Exam questions on Momentum and impulse in vector form

  1. A ball of mass 0.40.4 kg is moving with velocity (6i+8j)(6\mathbf{i}+8\mathbf{j}) m s−1^{-1} when it is hit by a bat. Immediately after being hit it moves with velocity (−2i+5j)(-2\mathbf{i}+5\mathbf{j}) m s−1^{-1}. The unit vectors i\mathbf{i} and j\mathbf{j} are perpendicular and lie in a horizontal plane.
    Find the angle between the direction of the impulse and the vector −i-\mathbf{i}.2 marks
  2. Two particles AA and BB, of masses 22 kg and 33 kg, move on a smooth horizontal plane and collide. Before the collision AA has velocity (4i−j)(4\mathbf{i}-\mathbf{j}) m s−1^{-1} and BB has velocity (−2i+3j)(-2\mathbf{i}+3\mathbf{j}) m s−1^{-1}. After the collision AA has velocity (−i+2j)(-\mathbf{i}+2\mathbf{j}) m s−1^{-1}. The unit vectors i\mathbf{i} and j\mathbf{j} are perpendicular and lie in the plane.
    Find the speed of BB after the collision.2 marks
  3. A tennis ball of mass 0.060.06 kg is moving with velocity (−20i+5j)(-20\mathbf{i}+5\mathbf{j}) m s−1^{-1} when it is struck by a racket. The racket exerts an impulse of (3i+1.5j)(3\mathbf{i}+1.5\mathbf{j}) N s on the ball. The unit vectors i\mathbf{i} and j\mathbf{j} are perpendicular and lie in a horizontal plane. Ignore the weight of the ball.
    Find the velocity of the ball immediately after it is struck.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).