Classical Dynamics of Particles and Systems · Problem 1-28

Newtonian Mechanics—Single Particle — Marion & Thornton

Physics — Mechanics · gradient-operator

Problem

Show that ∇(ln⁡∣r∣)=rr2\nabla(\ln|\mathbf{r}|) = \frac{\mathbf{r}}{r^2}
Intuitive explanation

This is about understanding how gradients work on scalar functions of position. The key insight is that ln⁡∣r∣\ln|\mathbf{r}| depends only on the distance rr from the origin, so you can use the chain rule: take the derivative with respect to rr, then multiply by ∇r\nabla r. Once you find ∇r=rr\nabla r = \frac{\mathbf{r}}{r}, the rest follows naturally from the chain rule applied to a radial function.

Intuitive explanation

This is about understanding how gradients work on scalar functions of position. The key insight is that ln⁡∣r∣\ln|\mathbf{r}| depends only on the distance rr from the origin, so you can use the chain rule: take the derivative with respect to rr, then multiply by ∇r\nabla r. Once you find ∇r=rr\nabla r = \frac{\mathbf{r}}{r}, the rest follows naturally from the chain rule applied to a radial function.

Related theory

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