Problem 36
Question
In Exercises \(31-38\) you will use a CAS to explore the osculating circle at a point \(P\) on a plane curve where \(\kappa \neq 0 .\) Use a CAS to perform the following steps: $$ \begin{array}{l}{\text { a. Plot the plane curve given in parametric or function form over }} \\ {\text { the specified interval to see what it looks like. }} \\ {\text { b. Calculate the curvature } \kappa \text { of the curve at the given value } t_{0}} \\ {\text { using the appropriate formula from Exercise } 5 \text { or } 6 . \text { Use the }} \\ {\text { parametrization } x=t \text { and } y=f(t) \text { if the curve is given as a }} \\ {\quad \text { function } y=f(x) \text { . }}\\\\{\text { c. Find the unit normal vector } N \text { at } t_{0} . \text { Notice that the signs of }} \\ {\text { the components of } N \text { depend on whether the unit tangent vector }} \\\ {\text { T is turning clockwise or counterclockwise at } t=t_{0} \text { . (See }} \\ {\text { Exercise } 7 . )}\\\\{\text { d. If } \mathbf{C}=a \mathbf{i}+b \mathbf{j} \text { is the vector from the origin to the center }(a, b)} \\ {\text { of the osculating circle, find the center } \mathbf{C} \text { from the vector }} \\ {\text { equation }} \\\ {\mathbf{C}=\mathbf{r}\left(t_{0}\right)+\frac{1}{\kappa\left(t_{0}\right)} \mathbf{N}\left(t_{0}\right)} \\ {\text { The point } P\left(x_{0}, y_{0}\right) \text { on the curve is given by the position }} \\ {\text { vector } \mathbf{r}\left(t_{0}\right) .}\\\\{\text { e. Plot implicitly the equation }(x-a)^{2}+(y-b)^{2}=1 / \kappa^{2}} \\ {\text { of the osculating circle. Then plot the curve and osculating }} \\ {\text { circle together. You may need to experiment with the size of }} \\ {\text { the viewing window, but be sure the axes are equally scaled. }}\end{array} $$ $$ \mathbf{r}(t)=\left(e^{-t} \cos t\right) \mathbf{i}+\left(e^{-t} \sin t\right) \mathbf{j}, \quad 0 \leq t \leq 6 \pi, \quad t_{0}=\pi / 4 $$
Step-by-Step Solution
VerifiedKey Concepts
Curvature Calculation
Here's how it works:
- First, find the first derivatives \( x' \) and \( y' \) of the parametric equations \( x(t) \) and \( y(t) \).
- Next, calculate the second derivatives \( x'' \) and \( y'' \).
- Use these derivatives in the curvature formula. This will give the curvature \( \kappa \) at a specific parameter value \( t_0 \), providing insight into the curve's bending."
Curvature is more than a number; it tells us how tight or loose a curve is bending at any point, similar to how radius works for circles. This geometric insight is important for understanding how curves behave.
Unit Normal Vector
The formula for \( \mathbf{T} \) is: \[ \mathbf{T}(t) = \frac{1}{\sqrt{x'^2 + y'^2}}(x' \mathbf{i} + y' \mathbf{j}) \]
- Compute \( \mathbf{T} \) using the derivatives \( x' \) and \( y' \).
- The unit normal vector \( \mathbf{N} \) is found by rotating \( \mathbf{T} \) by 90 degrees counterclockwise: \( \mathbf{N} = \langle -T_y, T_x \rangle \).
With the unit normal vector computed, it gives rise to the application in determining the center of the osculating circle. Understanding this orientation helps to know which direction the curve turns, contributing greatly to curve interviews and optimizations.
Parametric Equations
- \( x(t) = e^{-t} \cos t \)
- \( y(t) = e^{-t} \sin t \)
Parametric representation is especially useful when analyzing motion or other problems where the path and direction relate to time or another parameter. It provides clarity and precision where standard polynomial functions may fail.
Center of Osculating Circle
After calculating the position vector \( \mathbf{r}(t_0) \), the center \( \mathbf{C} \) of the osculating circle is determined by:\[ \mathbf{C} = \mathbf{r}(t_0) + \frac{1}{\kappa(t_0)} \mathbf{N}(t_0) \]
- Calculate \( \mathbf{r}(t_0) \), which gives the point \( P(x_0, y_0) \) on the curve.
- Use \( \mathbf{N}(t_0) \) and \( \kappa(t_0) \) to find the precise vector \( \mathbf{C} \).
This center point \( \mathbf{C} \), along with the radius \( 1/\kappa \), help construct the osculating circle, offering a deep understanding of the curve's immediate geometry. This circle not only aids in visualizing curvature but also finds applications in understanding movement dynamics and design.