Newton's Law of Gravitation — Question 10

Section 13-1 · Physics pages 1910–1911

Question 10 Central attraction can turn a velocity without changing angular momentum A particle of mass m at position⃗r relative to a fixed point source M feels⃗F = −GMm⃗r/r3. Its velocity need not be radial. M m r⃗ v⃗ F Instantaneous geometry; a transverse velocity does not by itself establish a circular orbit. (a) Find the torque about the source and deduce the behavior of angular momentum. (b) If the velocity is initially perpendicular to⃗r, determine the instantaneous power and explain why the acceleration is not zero.
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Question 10 - Solution Central attraction can turn a velocity without changing angular momentum M m r⃗ v⃗ F (a) Derivation and calculation For a fixed source,⃗ τ =⃗r ×⃗F = −GMm r3 (⃗r ×⃗r) =⃗0. Since d⃗L/dt =⃗τ,⃗ L =⃗r × m⃗v = constant . The force can change velocity without changing angular momentum about the source. (b) Result and interpretation At the specified instant⃗r ·⃗v = 0, so P =⃗F ·⃗v = −GMm r3⃗ r ·⃗v = 0 . Nevertheless,⃗ a = −GM r3⃗r̸ =⃗0 , d(v2) dt = 2⃗v ·⃗a = 0. Acceleration changes direction instantaneously; transverse velocity alone does not establish a circular orbit. Physical check The orbit is circular only if the transverse speed also satisfies v2 = GM/r.

Question 10

Central attraction can turn a velocity without changing angular momentum

A particle of mass mm at position r→\vec r relative to a fixed point source MM feels F→=−GMmr→/r3\vec F=-GMm\vec r/r^3. Its velocity need not be radial.

Diagram shown in the original SVG worksheet.

  1. Find the torque about the source and deduce the behavior of angular momentum.

  2. If the velocity is initially perpendicular to r→\vec r, determine the instantaneous power and explain why the acceleration is not zero.

Question 10 - Solution

Central attraction can turn a velocity without changing angular momentum

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For a fixed source, τ→=r→×F→=−GMmr3(r→×r→)=0→.\vec\tau=\vec r\times\vec F=-\frac{GMm}{r^3}(\vec r\times\vec r)=\vec0. Since dL→/dt=τ→d\vec L/dt=\vec\tau, L→=r→×mv→=constant.\boxed{\vec L=\vec r\times m\vec v=\text{constant}}. The force can change velocity without changing angular momentum about the source.

(b) Result and interpretation

At the specified instant r→⋅v→=0\vec r\cdot\vec v=0, so P=F→⋅v→=−GMmr3r→⋅v→=0.\boxed{P=\vec F\cdot\vec v=-\frac{GMm}{r^3}\vec r\cdot\vec v=0}. Nevertheless, a→=−GMr3r→≠0→,d(v2)dt=2v→⋅a→=0.\boxed{\vec a=-\frac{GM}{r^3}\vec r\ne\vec0},\qquad \frac{d(v^2)}{dt}=2\vec v\cdot\vec a=0. Acceleration changes direction instantaneously; transverse velocity alone does not establish a circular orbit.

Physical check

The orbit is circular only if the transverse speed also satisfies v2=GM/rv^2=GM/r.