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Find \(\mathbf{T}, \mathbf{N},\) and \(\kappa\) for the plane curves. \(\mathbf{r}(t)=t \mathbf{i}+(\ln \cos t) \mathbf{j}, \quad-\pi / 2< t< \pi / 2\)

Short Answer

Expert verified
\( \mathbf{T} = \cos(t) \mathbf{i} - \sin(t) \mathbf{j}, \mathbf{N} = -\sin(t) \mathbf{i} - \cos(t) \mathbf{j}, \kappa = \cos(t) \).

Step by step solution

01

Find the Derivative of the Position Vector

To find the tangent vector \( \mathbf{T} \), we start by finding the derivative of the position vector \( \mathbf{r}(t) \). The derivative is given by \( \mathbf{r}'(t) = \frac{d}{dt}[t] \mathbf{i} + \frac{d}{dt}[\ln(\cos t)] \mathbf{j} = \mathbf{i} - \tan(t) \mathbf{j} \).
02

Calculate the Magnitude of the Derivative

To normalize the tangent vector, we compute the magnitude of \( \mathbf{r}'(t) \). This is \( \| \mathbf{r}'(t) \| = \sqrt{1 + \tan^2(t)} = \sec(t) \).
03

Find the Unit Tangent Vector \( \mathbf{T} \)

The unit tangent vector is given by \( \mathbf{T}(t) = \frac{\mathbf{r}'(t)}{\| \mathbf{r}'(t) \|} = \cos(t) \mathbf{i} - \sin(t) \mathbf{j} \).
04

Find the Derivative of \( \mathbf{T}(t) \)

Differentiate \( \mathbf{T}(t) = \cos(t) \mathbf{i} - \sin(t) \mathbf{j} \). So, \( \mathbf{T}'(t) = -\sin(t) \mathbf{i} - \cos(t) \mathbf{j} \).
05

Calculate the Magnitude of \( \mathbf{T}'(t) \)

Compute the magnitude of \( \mathbf{T}'(t) \): \( \| \mathbf{T}'(t) \| = \sqrt{(-\sin(t))^2 + (-\cos(t))^2} = 1 \).
06

Find the Unit Normal Vector \( \mathbf{N} \)

The unit normal vector is given by \( \mathbf{N}(t) = \frac{\mathbf{T}'(t)}{\| \mathbf{T}'(t) \|} = -\sin(t) \mathbf{i} - \cos(t) \mathbf{j} \).
07

Compute Curvature \( \kappa \)

The curvature \( \kappa \) is given by \( \kappa = \frac{\| \mathbf{T}'(t) \|}{\| \mathbf{r}'(t) \|} = \cos(t) \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Tangent Vector
The tangent vector is a crucial concept when analyzing curves, as it represents the direction in which a curve is moving at any given point. For a curve described by the position vector \( \mathbf{r}(t) \), the tangent vector \( \mathbf{r}'(t) \) is the derivative of this position vector. The notation \( \frac{d}{dt} \) indicates differentiation with respect to the parameter \( t \).
For the given curve \( \mathbf{r}(t) = t \mathbf{i} + \ln(\cos t) \mathbf{j} \), its derivative, the tangent vector, is calculated as \( \mathbf{r}'(t) = \mathbf{i} - \tan(t) \mathbf{j} \).
This derivative gives the rate of change of the curve's position with time \( t \), essentially showing the direction of motion.
  • **Vector Components:** Shows how changes in \( t \) affect each part (\( \mathbf{i} \) and \( \mathbf{j} \) components).
  • **Slope Implication:** If \( \tan(t) \) varies, so does the curve's steepness or inclination.
Understanding the tangent vector helps comprehend the real-time dynamics of a curve.
Normal Vector
A normal vector is orthogonal, or perpendicular, to a tangent vector at a given point on a curve. This means that while the tangent vector shows the direction of the curve, the normal vector highlights the direction pointing outward from the curve's path. This concept is crucial for understanding how a curve is bending at any point.
To find the normal vector \( \mathbf{N}(t) \), one must first derive the unit tangent vector's derivative. For the provided curve, after normalizing, the derivative of \( \mathbf{T}(t) = \cos(t) \mathbf{i} - \sin(t) \mathbf{j} \) is \( \mathbf{T}'(t) = -\sin(t) \mathbf{i} - \cos(t) \mathbf{j} \).

**Unit Normal Vector:**
  • Calculated by normalizing \( \mathbf{T}'(t) \), the normal vector is expressed as \(-\sin(t) \mathbf{i} - \cos(t) \mathbf{j} \).
  • Having a magnitude of 1 ensures it is a "unit" vector—perfectly adapted to express pure direction without respect to length.
The normal vector provides insights into the curve’s bending away from the tangent, serving as a foundation for understanding curvature.
Unit Tangent Vector
A unit tangent vector, denoted \( \mathbf{T}(t) \), is a simplified version of the tangent vector. It has a length of 1. This makes it valuable for accurately representing direction without considering magnitude or length. To compute the unit tangent vector, divide the tangent vector by its magnitude, essentially normalizing it.
For example, from our calculation:

**Calculation Process:**
  • Given \( \mathbf{r}'(t) = \mathbf{i} - \tan(t) \mathbf{j} \), its magnitude, or length, is \( \| \mathbf{r}'(t) \| = \sec(t) \).
  • Then, the unit tangent vector is \( \mathbf{T}(t) = \frac{\mathbf{r}'(t)}{\| \mathbf{r}'(t) \|} = \cos(t) \mathbf{i} - \sin(t) \mathbf{j} \).
Using a unit tangent vector ensures a consistent and standardized way of assessing how the curve moves directionally, setting the stage for subsequent analyses like finding normal vectors and understanding curvature.

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Most popular questions from this chapter

In Exercises \(1-8,\) find the curve's unit tangent vector. Also, find the length of the indicated portion of the curve. $$ \mathbf{r}(t)=(t \sin t+\cos t) \mathbf{i}+(t \cos t-\sin t) \mathbf{j}, \quad \sqrt{2} \leq t \leq 2 $$

Firing from \(\left(x_{0}, y_{0}\right)\) Derive the equations $$ \begin{aligned} x &=x_{0}+\left(v_{0} \cos \alpha\right) t \\ y &=y_{0}+\left(v_{0} \sin \alpha\right) t-\frac{1}{2} g t^{2} \end{aligned} $$ (see Equation ( 5\()\) in the text) by solving the following initial value problem for a vector \(\mathbf{r}\) in the plane. $$ \begin{array}{ll}{\text { Differential equation: }} & {\frac{d^{2} \mathbf{r}}{d t^{2}}=-g \mathbf{j}} \\ {\text { Initial conditions: }} & {\mathbf{r}(0)=x_{0} \mathbf{i}+y_{0} \mathbf{j}} \\ {} & {\frac{d \mathbf{r}}{d t}(0)=\left(v_{0} \cos \alpha\right) \mathbf{i}+\left(v_{0} \sin \alpha\right) \mathbf{j}}\end{array} $$

Use a CAS to perform the following steps in Exercises \(58-61 .\) a. Plot the space curve traced out by the position vector \(\mathbf{r}\) . b. Find the components of the velocity vector \(d \mathbf{r} / d t\) . c. Evaluate \(d \mathbf{r} / d t\) at the given point \(t_{0}\) and determine the equation of the tangent line to the curve at \(\mathbf{r}\left(t_{0}\right) .\) d. Plot the tangent line together with the curve over the given interval. $$ \begin{array}{l}{\mathbf{r}(t)=\left(\ln \left(t^{2}+2\right)\right) \mathbf{i}+\left(\tan ^{-1} 3 t\right) \mathbf{j}+\sqrt{t^{2}+1} \mathbf{k}} \\\ {-3 \leq t \leq 5, \quad t_{0}=3}\end{array} $$

Hitting a baseball under a wind gust A baseball is hit when it is 2.5 \(\mathrm{ft}\) above the ground. It leaves the bat with an initial velocity of 145 \(\mathrm{ft} / \mathrm{sec}\) at a launch angle of \(23^{\circ} .\) At the instant the ball is hit, an instantaneous gust of wind blows against the ball, adding a component of \(-14 \mathbf{i}(\mathrm{ft} / \mathrm{sec})\) to the ball's initial velocity. A 15 -ft-high fence lies 300 \(\mathrm{ft}\) from home plate in the direction of the flight. a. Find a vector equation for the path of the baseball. b. How high does the baseball go, and when does it reach maximum height? c. Find the range and flight time of the baseball, assuming that the ball is not caught. d. When is the baseball 20 \(\mathrm{ft}\) high? How far (ground distance) is the baseball from home plate at that height? e. Has the batter hit a home run? Explain.

Products of scalar and vector functions Suppose that the scalar function \(u(t)\) and the vector function \(\mathbf{r}(t)\) are both defined for \(a \leq t \leq b\) . a. Show that \(u \mathbf{r}\) is continuous on \([a, b]\) if \(u\) and \(\mathbf{r}\) are continuous on \([a, b] .\) If \(u\) and \(\mathbf{r}\) are both differentiable on \([a, b],\) show that \(u \mathbf{r}\) is differentiable on \([a, b]\) and that $$ \frac{d}{d t}(u \mathbf{r})=u \frac{d \mathbf{r}}{d t}+\mathbf{r} \frac{d u}{d t} $$

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