2

Central Force Motion

medium25 pts

Statement#

A particle of mass mm moves under the influence of a central force F=f(r)r^\mathbf{F} = f(r)\hat{\mathbf{r}}, where f(r)f(r) is some function of the distance r=rr = |\mathbf{r}| from the origin, and r^=r/r\hat{\mathbf{r}} = \mathbf{r}/r is the unit radial vector.

Prove that the angular momentum L=r×p\mathbf{L} = \mathbf{r} \times \mathbf{p} is conserved (constant in time).

Required Topics#

  • Newton's second law
  • Central forces
  • Angular momentum
  • Vector cross products
  • Time derivatives of vector quantities
  • Conservation laws

Definitions#

Central Force: A force directed along the line connecting the particle to the origin: F=f(r)r^\mathbf{F} = f(r)\hat{\mathbf{r}}

Angular Momentum: L=r×p=r×mv\mathbf{L} = \mathbf{r} \times \mathbf{p} = \mathbf{r} \times m\mathbf{v}

What to Prove#

Show that dLdt=0\frac{d\mathbf{L}}{dt} = \mathbf{0}, which means angular momentum is conserved.

Key Identity#

Product rule for cross products: ddt(A×B)=dAdt×B+A×dBdt\frac{d}{dt}(\mathbf{A} \times \mathbf{B}) = \frac{d\mathbf{A}}{dt} \times \mathbf{B} + \mathbf{A} \times \frac{d\mathbf{B}}{dt}

Solution#

Solution coming soon.

Hints (4)

Topics Needed

central-forcesangular-momentumconservation-laws

Prerequisites

  • newton-laws
  • vector-calculus
  • cross-products

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