Problem 45
Question
In Exercises \(43 - 46 ,\) use a CAS to perform the following steps to evaluate the line integrals. $$ \begin{array} { l } { \text { a. Find } d s = | \mathbf { v } ( t ) | d t \text { for the path } \mathbf { r } ( t ) = g ( t ) \mathbf { i } + h ( t ) \mathbf { j } + k ( t ) \mathbf { k } \text { . } } \\ { \text { b. Express the integrand } f ( g ( t ) , h ( t ) , k ( t ) ) | \mathbf { v } ( t ) | \text { as a function of the parameter } t . } \\ { \text { c. Evaluate } \int _ { C } f d s \text { using Equation } ( 2 ) \text { in the text. } } \end{array} $$ $$ \begin{array} { l } { f ( x , y , z ) = x \sqrt { y } - 3 z ^ { 2 } ; \quad \mathbf { r } ( t ) = ( \cos 2 t ) \mathbf { i } + ( \sin 2 t ) \mathbf { j } + 5 t \mathbf { k } } \\ { 0 \leq t \leq 2 \pi } \end{array} $$
Step-by-Step Solution
VerifiedKey Concepts
Vector Calculus
Line integrals have two types: path integrals (which involve scalar fields) and circulation integrals (which involve vector fields). Using vector calculus, we analyze these integrals by breaking them down into vector components. This is particularly important in physics, where fields are often represented as vector fields.
By incorporating functions that go beyond simple scalar fields, vector calculus allows for the evaluation of integrals in multidimensional spaces. It is vital to understand how to apply vector calculus when dealing with complex paths, especially in the case of curves or surfaces.
Parameterization of Curves
For instance, in this problem, the curve is parameterized by the function \( \mathbf{r}(t) = (\cos 2t) \mathbf{i} + (\sin 2t) \mathbf{j} + 5t \mathbf{k} \). This representation not only informs the shape and orientation of the path but also specifies how a point travels along the curve as \( t \) varies from 0 to \( 2\pi \). By using trigonometric functions and polynomial expressions, we can describe intricate paths that traverse through three-dimensional space.
To successfully parameterize a curve, the chosen functions must continuously cover the interval of interest. For example, using sine and cosine for circular paths ensures smooth traversal across the curve while also facilitating easier computations in later stages. Parameterization thus simplifies integral evaluations by transforming them into an easier-to-analyze form of the parameter \( t \).
Differentiation of Vector Functions
Differentiating a vector function involves taking the derivative of each component separately. For the given path \( \mathbf{r}(t) = (\cos 2t) \mathbf{i} + (\sin 2t) \mathbf{j} + 5t \mathbf{k} \), its differentiation yields:
- A derivative of \( \cos 2t \) with respect to \( t \) gives \(-2\sin 2t \),
- A derivative of \( \sin 2t \) gives \( 2\cos 2t \), and
- A derivative of \( 5t \) naturally gives 5.
Understanding how to differentiate vector functions is critical in physics for determining rates of change, such as velocity or acceleration, which in turn can describe motions of particles or objects along a trajectory.
Magnitude of a Vector
In this problem, the magnitude of the velocity vector \( \mathbf{v}(t) = (-2\sin 2t) \mathbf{i} + (2\cos 2t) \mathbf{j} + 5 \mathbf{k} \) is vital for integrating along the curve. We compute it by applying the Pythagorean theorem, which in multiple dimensions involves summing the squares of all components:
- \((-2\sin 2t)^2\) contributes \(4\sin^2 2t\),
- \((2\cos 2t)^2\) gives \(4\cos^2 2t\), and
- The constant \(5^2\) equals 25.
Understanding vector magnitudes is crucial in scenarios requiring calculations of distances or lengths, such as in physics for traversing paths, or in geometry and graphics for scaling transformations.