Newton's Second Law in Angular Form — Question 1

Section 11-7 · Physics pages 1672–1673

Question 1 The angular equation follows from a product rule A particle of constant mass m has position⃗r, velocity⃗v and momentum⃗p = m⃗v, all measured relative to a fixed inertial origin. O fixed⃗ r⃗ p = m⃗v⃗ F = ˙⃗p A fixed-origin position and the particle momentum define angular momentum; the force changes it. (a) Derive d⃗L/dt =⃗τ from⃗L =⃗r ×⃗p. (b) Explain why⃗v ×⃗p disappears and why a moving origin needs extra care.
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Question 1 - Solution The angular equation follows from a product rule O fixed⃗ r⃗ p = m⃗v⃗ F = ˙⃗p (a) Derivation and calculation Apply the product rule to⃗L =⃗r ×⃗p: d⃗L dt = d⃗r dt ×⃗p +⃗r × d⃗p dt . At a fixed inertial origin, ˙⃗r =⃗v and⃗p = m⃗v, so⃗ v ×⃗p = m⃗v ×⃗v =⃗0. Newton’s law therefore gives d⃗L dt =⃗r ×⃗F =⃗τ . (b) Result and interpretation For an origin A moving at velocity⃗VA, relative position has derivative⃗v −⃗VA. If angular momentum uses inertial momentum, d⃗LA dt = (⃗v −⃗VA) ×⃗p +⃗rP/A ×⃗F =⃗τA −⃗VA ×⃗p . The extra term cannot generally be dropped; the choice of both position origin and momentum frame matters. Physical check The fixed-origin law follows when⃗VA = 0; the added term also vanishes when⃗VA is parallel to momentum.

Question 1

The angular equation follows from a product rule

A particle of constant mass mm has position r→\vec r, velocity v→\vec v and momentum p→=mv→\vec p=m\vec v, all measured relative to a fixed inertial origin.

Diagram shown in the original SVG worksheet.

  1. Derive dL→/dt=τ→d\vec L/dt=\vec\tau from L→=r→×p→\vec L=\vec r\times\vec p.

  2. Explain why v→×p→\vec v\times\vec p disappears and why a moving origin needs extra care.

Question 1 - Solution

The angular equation follows from a product rule

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Apply the product rule to L→=r→×p→\vec L=\vec r\times\vec p: dL→dt=dr→dt×p→+r→×dp→dt.\frac{d\vec L}{dt}=\frac{d\vec r}{dt}\times\vec p+\vec r\times\frac{d\vec p}{dt}. At a fixed inertial origin, r→̇=v→\dot{\vec r}=\vec v and p→=mv→\vec p=m\vec v, so v→×p→=mv→×v→=0→.\vec v\times\vec p=m\vec v\times\vec v=\vec0. Newton’s law therefore gives dL→dt=r→×F→=τ→.\boxed{\frac{d\vec L}{dt}=\vec r\times\vec F=\vec\tau}.

(b) Result and interpretation

For an origin AA moving at velocity V→A\vec V_A, relative position has derivative v→−V→A\vec v-\vec V_A. If angular momentum uses inertial momentum, dL→Adt=(v→−V→A)×p→+r→P/A×F→=τ→A−V→A×p→.\frac{d\vec L_A}{dt}=(\vec v-\vec V_A)\times\vec p+\vec r_{P/A}\times\vec F =\boxed{\vec\tau_A-\vec V_A\times\vec p}. The extra term cannot generally be dropped; the choice of both position origin and momentum frame matters.

Physical check

The fixed-origin law follows when V→A=0\vec V_A=0; the added term also vanishes when V→A\vec V_A is parallel to momentum.