Section Objectives
The derivative of a vector-valued function is defined by a limit,
just like the derivative you saw in Calculus I. However, since we evaluate limits of vector-valued functions component by component, it is probably not surprising to you that we can evaluate derivatives in a similar way:
Suppose , and are differentiable functions of , and further suppose that is a constant.
Each of these properties is easy to prove. Unfortunately, because we will usually compute our derivatives component by component, we will not find these properties very useful. Property 7 is an exception---we will use this property often.
Recall that the derivative of a scalar-valued function gives the slope of the tangent line. For vector-valued functions, the derivative gives a tangent vector.
In the graph above, the tangent vector shown is in fact a unit vector. It is a unit tangent vector.
Suppose is a curve in space defined by the vector-valued function . Assume exists and is not the zero vector. Then the principal unit tangent vector at is given by
If we think of as giving the position of a particle at time , then is the unit vector that points in the direction of motion.
As with limits and derivatives, we evaluate the integral of a vector-valued function component by component. That is, the integral of a vector-valued function is obtained by integrating each component:
For indefinite integrals, it is very important to include a scalar constant of integration with each component. Alternatively, you can include a vector constant of integration for the entire integral.