Find the tangent vector at a point for a given position vector
Find and interpret unit tangent vectors
Calculate the definite integral of a vector-valued function
Derivatives of Vector-Valued Functions
To study the calculus of vector-valued functions, we follow a path similar to real-valued functions: define the derivative, examine applications, then move on to integrals. The vector nature of these functions brings some interesting new ideas along the way.
Now that you know what a vector-valued function is and how to take its limit, the next step is learning to differentiate it. The definition closely parallels the derivative of a real-valued function, but because the range consists of vectors, the derivative is also a vector.
derivative of a vector-valued function
The derivative of a vector-valued function [latex]{\bf{r}}(t)[/latex] is
Just as with real-valued functions, the derivative of a vector-valued function represents an instantaneous rate of change. When the function represents the position of an object at time [latex]t[/latex], the derivative represents its velocity at that same moment.
Use the definition to calculate the derivative of the function
Calculating derivatives using the limit definition works, but it’s tedious. Fortunately, we can differentiate component by component—just like we handled limits.
differentiation of vector-valued functions theorem
Let [latex]f[/latex], [latex]g[/latex], and [latex]h[/latex] be differentiable functions of [latex]t[/latex].
If [latex]{\bf{r}}\,(t)=f\,(t)\,{\bf{i}}+g\,(t)\,{\bf{j}}[/latex], then [latex]{\bf{r}}'\,(t)=f'\,(t)\,{\bf{i}}+g'\,(t)\,{\bf{j}}[/latex].
If [latex]{\bf{r}}\,(t)=f\,(t)\,{\bf{i}}+g\,(t)\,{\bf{j}}+h\,(t)\,{\bf{k}}[/latex], then [latex]{\bf{r}}'\,(t)=f'\,(t)\,{\bf{i}}+g'\,(t)\,{\bf{j}}+h'\,(t)\,{\bf{k}}[/latex].
Differentiate each component separately using the derivative rules you already know from Calculus 1. The vector structure doesn’t change—only the components do.
Since we will be using derivatives of common single-variable functions throughout this course, we briefly recall the derivatives of common functions, along with frequently-encountered derivative rules below.
We use Differentiation of Vector-Valued Functions and what we know about differentiating functions of one variable.
The first component of [latex]{\bf{r}}\,(t)=(6t+8)\,{\bf{i}}+(4t^{2}+2t-3)\,{\bf{j}}[/latex] is [latex]f\,(t)=6t+8[/latex]. The second component is [latex]g\,(t)=4t^{2}+2t-3[/latex]. We have [latex]f'\,(t)=6[/latex] and [latex]g'\,(t)=8t+2[/latex], so the theorem gives [latex]{\bf{r}}'\,(t)=6\,{\bf{i}}+(8t+2)\,{\bf{j}}[/latex]
The first component is [latex]f\,(t)=3\cos{t}[/latex] and the second component is [latex]g\,(t)=4\sin{t}[/latex]. We have [latex]f'\,(t)=-3\sin{t}[/latex] and [latex]g'\,(t)=4\cos{t}[/latex], so we obtain [latex]{\bf{r}}'\,(t)=-3\sin{t\,{\bf{i}}}+4\cos{t\,{\bf{j}}}[/latex]
The first component of [latex]{\bf{r}}\,(t)=e^{t}\sin{t\,{\bf{i}}}+e^{t}\cos{t{\bf{j}}}-e^{2t}\,{\bf{k}}[/latex] is [latex]f\,(t)=e^{t}\sin{t}[/latex], the second component is [latex]g\,(t)=e^{t}\cos{t}[/latex], and the third component is [latex]h\,(t)=-e^{2t}[/latex]. We have [latex]f'\,(t)=e^{t}(\sin{t}+\cos{t}),\ g'\,(t)=e^{t}(\cos{t}-\sin{t})[/latex], and [latex]h'\,(t)=-2e^{2t}[/latex], so the theorem gives [latex]{\bf{r}}'\,(t)=e^{t}(\sin{t}+\cos{t})\,{\bf{i}}+e^{t}(\cos{t}-\sin{t})\,{\bf{j}}-2e^{2t}\,{\bf{k}}[/latex]
Properties of Derivatives
The derivative properties you learned in Calculus 1 extend to vector-valued functions. The constant multiple rule, sum and difference rules, and chain rule all work the same way. The product rule has three versions because vectors can be multiplied in three different ways: scalar multiplication, dot product, and cross product.
differentiation rules for vector-valued functions
Let [latex]{\bf{r}}[/latex] and [latex]{\bf{u}}[/latex] be differentiable vector-valued functions of [latex]t[/latex], and let [latex]f[/latex] be a differentiable real-valued function of [latex]t[/latex]. Let [latex]c[/latex] be a scalar.
If [latex]{\bf{r}},(t)\cdot{\bf{r}},(t)=c[/latex], then [latex]{\bf{r}},(t)\cdot{\bf{r}}',(t)=0[/latex]
Proof
The proofs of the first two properties follow directly from the definition of the derivative of a vector-valued function. The third property can be derived from the first two properties, along with the product rule from the Introduction to Derivatives. Let [latex]{\bf{u}}\,(t)=g\,(t)\,{\bf{i}}+h\,(t)\,{\bf{j}}[/latex]. Then
To prove property 4. Let [latex]{\bf{r}}\,(t)=f_{1}\,(t)\,{\bf{i}}+g_{1}\,(t)\,{\bf{j}}[/latex] and [latex]{\bf{u}}\,(t)=f_{2}\,(t)\,{\bf{i}}+g_{2}\,(t)\,{\bf{j}}[/latex]. Then
We have [latex]{\bf{r}}'\,(t)=6\,{\bf{i}}+(8t+2)\,{\bf{j}}+5\,{\bf{k}}[/latex] and [latex]{\bf{u}}'\,(t)=2t\,{\bf{i}}+2\,{\bf{j}}+(3t^{2}-3)\,{\bf{k}}[/latex]. Therefore, according to property 4:
Recall that the cross product of any vector with itself is zero. Furthermore, [latex]{\bf{u}}''\,(t)[/latex] represents the second derivative of [latex]{\bf{u}}\,(t)[/latex]: