Derivative of a Vector Function

Differentiate r(t) component by component, then get velocity, speed and the unit tangent
Derivative of r(t) = <t^2, sin(t), e^(3t)>
Unit tangent vector for r(t) = <cos t, sin t, t> at t = pi/2
Derivative of the dot product of <t, t^2, 1> and <1, t, t^3>
Speed of a particle with r(t) = <3t, 4t, 5>

Differentiate Component by Component

A vector-valued function r(t)=โŸจf(t),โ€‰g(t),โ€‰h(t)โŸฉ\mathbf{r}(t) = \langle f(t),\, g(t),\, h(t)\rangle traces a curve in space as tt varies. Its derivative comes from the same limit as in single-variable calculus,

rโ€ฒ(t)=limโกฮ”tโ†’0r(t+ฮ”t)โˆ’r(t)ฮ”t\mathbf{r}'(t) = \lim_{\Delta t \to 0}\frac{\mathbf{r}(t + \Delta t) - \mathbf{r}(t)}{\Delta t}

and because vector subtraction and scalar division act componentwise, this collapses to the rule you actually use:

rโ€ฒ(t)=โŸจfโ€ฒ(t),โ€‰gโ€ฒ(t),โ€‰hโ€ฒ(t)โŸฉ\mathbf{r}'(t) = \langle f'(t),\, g'(t),\, h'(t)\rangle

It exists only where every component is differentiable โ€” one non-smooth component kills the whole derivative.

What it means geometrically. rโ€ฒ(t)\mathbf{r}'(t) is a vector, not a slope: it points along the curve in the direction of increasing tt and is tangent to it. If r\mathbf{r} is position, then rโ€ฒ\mathbf{r}' is velocity, โˆฅrโ€ฒโˆฅ\|\mathbf{r}'\| is speed (a scalar), and rโ€ฒโ€ฒ\mathbf{r}'' is acceleration.

Rules, Speed and the Unit Tangent

With u,v\mathbf{u}, \mathbf{v} differentiable and cc a scalar function:

ddt[u+v]=uโ€ฒ+vโ€ฒ,ddt[cโ€‰u]=cโ€ฒu+cโ€‰uโ€ฒ\frac{d}{dt}[\mathbf{u} + \mathbf{v}] = \mathbf{u}' + \mathbf{v}', \qquad \frac{d}{dt}[c\,\mathbf{u}] = c'\mathbf{u} + c\,\mathbf{u}'

ddt[uโ‹…v]=uโ€ฒโ‹…v+uโ‹…vโ€ฒ(aย scalar)\frac{d}{dt}[\mathbf{u} \cdot \mathbf{v}] = \mathbf{u}' \cdot \mathbf{v} + \mathbf{u} \cdot \mathbf{v}' \quad (\text{a scalar})

ddt[uร—v]=uโ€ฒร—v+uร—vโ€ฒ(orderย isย fixed)\frac{d}{dt}[\mathbf{u} \times \mathbf{v}] = \mathbf{u}' \times \mathbf{v} + \mathbf{u} \times \mathbf{v}' \quad (\text{order is fixed})

ddt[r(s(t))]=rโ€ฒ(s(t))โ€‰sโ€ฒ(t)\frac{d}{dt}[\mathbf{r}(s(t))] = \mathbf{r}'(s(t))\,s'(t)

Speed is the magnitude โˆฅrโ€ฒ(t)โˆฅ=fโ€ฒ2+gโ€ฒ2+hโ€ฒ2\|\mathbf{r}'(t)\| = \sqrt{f'^2 + g'^2 + h'^2}, and arc length on [a,b][a,b] is โˆซabโˆฅrโ€ฒ(t)โˆฅโ€‰dt\int_a^b \|\mathbf{r}'(t)\|\,dt.

The unit tangent requires rโ€ฒ(t)โ‰ 0\mathbf{r}'(t) \neq \mathbf{0}:

T(t)=rโ€ฒ(t)โˆฅrโ€ฒ(t)โˆฅ\mathbf{T}(t) = \frac{\mathbf{r}'(t)}{\|\mathbf{r}'(t)\|}

A curve with rโ€ฒโ‰ 0\mathbf{r}' \neq \mathbf{0} everywhere is called smooth; where rโ€ฒ=0\mathbf{r}' = \mathbf{0} the curve can have a cusp even though every component is differentiable.

Common Mistakes to Avoid

  • Reversing a cross product. uโ€ฒร—v+uร—vโ€ฒ\mathbf{u}' \times \mathbf{v} + \mathbf{u} \times \mathbf{v}' โ€” swapping either factor flips a sign, because aร—b=โˆ’โ€‰bร—a\mathbf{a} \times \mathbf{b} = -\,\mathbf{b} \times \mathbf{a}.
  • Confusing โˆฅrโˆฅโ€ฒ\|\mathbf{r}\|' with โˆฅrโ€ฒโˆฅ\|\mathbf{r}'\|. They are different: for r=โŸจcosโกt,sinโกtโŸฉ\mathbf{r} = \langle\cos t, \sin t\rangle the first is 00 and the second is 11.
  • Treating rโ€ฒ\mathbf{r}' as a slope. It is a vector; the "slope" of a space curve is not defined.
  • Forgetting the chain rule inside a component. ddte3t=3e3t\frac{d}{dt}e^{3t} = 3e^{3t}, not e3te^{3t}.
  • Normalising before differentiating. Tโ€ฒ(t)\mathbf{T}'(t) is not rโ€ฒโ€ฒ/โˆฅrโ€ฒโ€ฒโˆฅ\mathbf{r}''/\|\mathbf{r}''\|; differentiate r\mathbf{r} first, then normalise.
  • Dividing by zero at a cusp. Check rโ€ฒ(t)โ‰ 0\mathbf{r}'(t) \neq \mathbf{0} before forming T(t)\mathbf{T}(t).

Examples

Step 1: Differentiate each component separately
Step 2: First: ddtt2=2t\dfrac{d}{dt}t^2 = 2t
Step 3: Second: ddtsinโกt=cosโกt\dfrac{d}{dt}\sin t = \cos t
Step 4: Third (chain rule): ddte3t=3e3t\dfrac{d}{dt}e^{3t} = 3e^{3t}
Answer: rโ€ฒ(t)=โŸจ2t,โ€…โ€Šcosโกt,โ€…โ€Š3e3tโŸฉ\mathbf{r}'(t) = \langle 2t,\; \cos t,\; 3e^{3t}\rangle

Step 1: rโ€ฒ(t)=โŸจโˆ’sinโกt,โ€…โ€Šcosโกt,โ€…โ€Š1โŸฉ\mathbf{r}'(t) = \langle -\sin t,\; \cos t,\; 1\rangle
Step 2: โˆฅrโ€ฒ(t)โˆฅ=sinโก2t+cosโก2t+1=1+1=2\|\mathbf{r}'(t)\| = \sqrt{\sin^2 t + \cos^2 t + 1} = \sqrt{1 + 1} = \sqrt{2} โ€” constant speed
Step 3: At t=ฯ€/2t = \pi/2: rโ€ฒ(ฯ€/2)=โŸจโˆ’1,โ€…โ€Š0,โ€…โ€Š1โŸฉ\mathbf{r}'(\pi/2) = \langle -1,\; 0,\; 1\rangle
Step 4: T=12โŸจโˆ’1,โ€…โ€Š0,โ€…โ€Š1โŸฉ\mathbf{T} = \dfrac{1}{\sqrt{2}}\langle -1,\; 0,\; 1\rangle
Answer: Speed =2= \sqrt{2}; T(ฯ€/2)=โŸจโˆ’12,โ€…โ€Š0,โ€…โ€Š12โŸฉ\mathbf{T}(\pi/2) = \left\langle -\tfrac{1}{\sqrt{2}},\; 0,\; \tfrac{1}{\sqrt{2}}\right\rangle

Step 1: uโ€ฒ=โŸจ1,โ€‰2t,โ€‰0โŸฉ\mathbf{u}' = \langle 1,\, 2t,\, 0\rangle and vโ€ฒ=โŸจ0,โ€‰1,โ€‰3t2โŸฉ\mathbf{v}' = \langle 0,\, 1,\, 3t^2\rangle
Step 2: uโ€ฒโ‹…v=(1)(1)+(2t)(t)+(0)(t3)=1+2t2\mathbf{u}' \cdot \mathbf{v} = (1)(1) + (2t)(t) + (0)(t^3) = 1 + 2t^2
Step 3: uโ‹…vโ€ฒ=(t)(0)+(t2)(1)+(1)(3t2)=4t2\mathbf{u} \cdot \mathbf{v}' = (t)(0) + (t^2)(1) + (1)(3t^2) = 4t^2
Step 4: Add: 1+2t2+4t2=1+6t21 + 2t^2 + 4t^2 = 1 + 6t^2
Step 5: Check directly: uโ‹…v=t+t3+t3=t+2t3\mathbf{u} \cdot \mathbf{v} = t + t^3 + t^3 = t + 2t^3, whose derivative is 1+6t21 + 6t^2
Answer: 1+6t21 + 6t^2 (a scalar)

Frequently Asked Questions

Differentiate each component with respect to the parameter and reassemble them into a vector. For r(t) = <f, g, h> the derivative is r'(t) = <f', g', h'>. No new technique is needed beyond ordinary single-variable differentiation.

It is the tangent vector to the curve, pointing in the direction of increasing t. If r(t) is position then r'(t) is velocity, its magnitude is the speed, and r''(t) is acceleration.

Yes, and both look like the ordinary product rule. The dot version gives a scalar. The cross version requires you to preserve the order of the factors, since the cross product is anticommutative.

T(t) = r'(t)/||r'(t)|| is undefined wherever r'(t) is the zero vector, because you would divide by zero. Such points are where the curve can have a cusp, even if each component function is perfectly differentiable.

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