Differentiation

Work in progress. This note is still being written and incomplete.

2 min read Last updated Fri Aug 14 2026 03:05:03 GMT+0000 (Coordinated Universal Time)

The derivative of r\boldsymbol{r} is defined the same way as for a real-valued function:

r(t)=dr(t)dt=limh0r(t+h)r(t)h\boldsymbol{r}'(t) = \frac{\text{d}\boldsymbol{r}(t)}{\text{d}t} = \lim_{h \to 0} \frac{\boldsymbol{r}(t+h) - \boldsymbol{r}(t)}{h}

provided the limit exists.

For r(t)=x(t),y(t),z(t)\boldsymbol{r}(t) = \langle x(t), y(t), z(t) \rangle, r\boldsymbol{r} is differentiable at aa iff each component function is differentiable at aa, and

r(a)=x(a),y(a),z(a)\boldsymbol{r}'(a) = \langle x'(a), y'(a), z'(a) \rangle

More generally, whenever the component derivatives exist,

r(t)=x(t),y(t),z(t)\boldsymbol{r}'(t) = \langle x'(t), y'(t), z'(t) \rangle

For differentiable vector-valued functions r(t)\boldsymbol{r}(t), r1(t)\boldsymbol{r}_1(t), r2(t)\boldsymbol{r}_2(t), differentiable real-valued function f(t)f(t), scalar kk, and constant vector c\vec{c}:

  • ddt[c]=0\dfrac{\text{d}}{\text{d}t}[\vec{c}] = \vec{0}
  • ddt[r1(t)±r2(t)]=r1(t)±r2(t)\dfrac{\text{d}}{\text{d}t}[\boldsymbol{r}_1(t) \pm \boldsymbol{r}_2(t)] = \boldsymbol{r}_1'(t) \pm \boldsymbol{r}_2'(t)
  • ddt[kr(t)]=kr(t)\dfrac{\text{d}}{\text{d}t}[k\boldsymbol{r}(t)] = k\boldsymbol{r}'(t)
  • ddt[f(t)r(t)]=f(t)r(t)+f(t)r(t)\dfrac{\text{d}}{\text{d}t}[f(t)\boldsymbol{r}(t)] = f(t)\boldsymbol{r}'(t) + f'(t)\boldsymbol{r}(t)
  • ddt[r1(t)r2(t)]=r1(t)[r2(t)+r1(t)r2(t)\dfrac{\text{d}}{\text{d}t}[\boldsymbol{r}_1(t) \cdot \boldsymbol{r}_2(t)] = \boldsymbol{r}_1(t) \cdot [\boldsymbol{r}_2'(t) + \boldsymbol{r}_1'(t) \cdot \boldsymbol{r}_2(t)
  • ddt[r1(t)×r2(t)]=r1(t)×[r2(t)+r1(t)×r2(t)\dfrac{\text{d}}{\text{d}t}[\boldsymbol{r}_1(t) \times \boldsymbol{r}_2(t)] = \boldsymbol{r}_1(t) \times [\boldsymbol{r}_2'(t) + \boldsymbol{r}_1'(t) \times \boldsymbol{r}_2(t)
  • ddt[r(f(t))]=f(t)r(f(t))\dfrac{\text{d}}{\text{d}t}[\boldsymbol{r}(f(t))] = f'(t)\boldsymbol{r}'(f(t))

Tangent Line

Let PP be a point on the graph of r(t)\boldsymbol{r}(t), with r(t0)\boldsymbol{r}(t_0) the position vector of PP. If r(t0)\boldsymbol{r}'(t_0) exists and is non-zero, r(t0)\boldsymbol{r}'(t_0) is a tangent vector to the graph at PP. The tangent line through PP parallel to r(t0)\boldsymbol{r}'(t_0) has vector equation

x(s)=r(t0)+sr(t0),sR\vec{x}(s) = \boldsymbol{r}(t_0) + s\boldsymbol{r}'(t_0), \qquad s \in \mathbb{R}

If r(t)\lVert \boldsymbol{r}(t) \rVert is constant for all tt in an interval, then r(t)r(t)=0\boldsymbol{r}(t) \cdot \boldsymbol{r}'(t) = 0. So r(t)\boldsymbol{r}(t) and r(t)\boldsymbol{r}'(t) are orthogonal for every tt in the interval.

Mean Value Theorem

Vector-valued functions do not satisfy a direct Mean Value Theorem of the form r(b)r(a)=r(c)(ba)\boldsymbol{r}(b) - \boldsymbol{r}(a) = \boldsymbol{r}'(c)(b-a).

Was this helpful?