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Find \(\mathbf{T}, \mathbf{N},\) and \(\kappa\) for the space curves $$ \mathbf{r}(t)=(\cosh t) \mathbf{i}-(\sinh t) \mathbf{j}+t \mathbf{k} $$

Short Answer

Expert verified
\( \mathbf{T}(t) = \frac{1}{\sqrt{2}}(\sinh t \mathbf{i} - \cosh t \mathbf{j} + \mathbf{k}) \), \( \mathbf{N}(t) = \frac{1}{\sqrt{2}}(\cosh t \mathbf{i} + \sinh t \mathbf{j}) \), \( \kappa(t) = \frac{1}{2\sqrt{2}} \).

Step by step solution

01

Compute the First Derivative

Find the derivative \( \mathbf{r}'(t) \) of the curve \( \mathbf{r}(t) = (\cosh t) \mathbf{i} - (\sinh t) \mathbf{j} + t \mathbf{k} \). The derivatives are \( \frac{d}{dt}(\cosh t) = \sinh t \), \( \frac{d}{dt}(-\sinh t) = -\cosh t \), and \( \frac{d}{dt}(t) = 1 \). Thus, \( \mathbf{r}'(t) = (\sinh t) \mathbf{i} - (\cosh t) \mathbf{j} + \mathbf{k} \).
02

Calculate the Unit Tangent Vector

The unit tangent vector \( \mathbf{T}(t) \) is given by \( \mathbf{T}(t) = \frac{\mathbf{r}'(t)}{\|\mathbf{r}'(t)\|} \). First, find \( \|\mathbf{r}'(t)\| \) as follows: \( \|\mathbf{r}'(t)\| = \sqrt{(\sinh t)^2 + (\cosh t)^2 + 1^2} \). Use the identity \( \cosh^2 t - \sinh^2 t = 1 \) to simplify this as \( \|\mathbf{r}'(t)\| = \sqrt{1 + 1} = \sqrt{2} \). Therefore, \( \mathbf{T}(t) = \frac{1}{\sqrt{2}}((\sinh t) \mathbf{i} - (\cosh t) \mathbf{j} + \mathbf{k}) \).
03

Obtain the Second Derivative

Find the second derivative \( \mathbf{r}''(t) \) of the function to proceed. We have \( \frac{d}{dt}(\sinh t) = \cosh t \) and \( \frac{d}{dt}(-\cosh t) = -\sinh t \). Thus, \( \mathbf{r}''(t) = (\cosh t) \mathbf{i} + (\sinh t) \mathbf{j} \).
04

Compute the Normal Vector

Calculate \( \mathbf{T}'(t) = \frac{d}{dt}\left(\frac{1}{\sqrt{2}}(\sinh t \mathbf{i} - \cosh t \mathbf{j} + \mathbf{k})\right) \). After differentiating, we have \( \mathbf{T}'(t) = \frac{1}{\sqrt{2}}(\cosh t \mathbf{i} + \sinh t \mathbf{j}) \).
05

Find the Unit Normal Vector

The unit normal vector \( \mathbf{N}(t) \) is given by \( \mathbf{N}(t) = \frac{\mathbf{T}'(t)}{\|\mathbf{T}'(t)\|} \). Note that \( \|\mathbf{T}'(t)\| = \frac{1}{\sqrt{2}}\sqrt{(\cosh t)^2 + (\sinh t)^2} = 1 \). Hence, \( \mathbf{N}(t) = \mathbf{T}'(t) = \frac{1}{\sqrt{2}}(\cosh t \mathbf{i} + \sinh t \mathbf{j}) \).
06

Calculate the Curvature

The curvature \( \kappa(t) \) is given by \( \kappa(t) = \frac{\|\mathbf{r}''(t) \times \mathbf{r}'(t)\|}{\|\mathbf{r}'(t)\|^3} \). Compute the cross product \( \mathbf{r}''(t) \times \mathbf{r}'(t) \). Using \( \mathbf{r}''(t) = \cosh t \mathbf{i} + \sinh t \mathbf{j} \) and \( \mathbf{r}'(t) = \sinh t \mathbf{i} - \cosh t \mathbf{j} + \mathbf{k} \):\[\mathbf{r}''(t) \times \mathbf{r}'(t) = \left|\begin{array}{ccc}\mathbf{i} & \mathbf{j} & \mathbf{k} \\cosh t & \sinh t & 0 \\sinh t & -\cosh t & 1\end{array}\right| = \left\|\begin{array}{cc}\sinh t & 0 \\-\cosh t & 1\end{array}\right\| \mathbf{i} + \left\|\begin{array}{cc}\cosh t & 0 \\sinh t & 1\end{array}\right\| \mathbf{j} + \left\|\begin{array}{cc}\cosh t & \sinh t \\sinh t & -\cosh t\end{array}\right\| \mathbf{k} \]The resulting calculation leads to \( \mathbf{k} \), thus \( \|\mathbf{r}''(t) \times \mathbf{r}'(t)\| = 1 \). Finally, compute \( \kappa(t) = \frac{1}{(\sqrt{2})^3} = \frac{1}{2\sqrt{2}} \).

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Key Concepts

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

Unit Tangent Vector
In differential geometry, the unit tangent vector provides essential information about a curve's direction at a particular point. To find the unit tangent vector for a space curve, we start by taking the derivative of the position vector
  • The position vector, given by \( \mathbf{r}(t) = (\cosh t) \mathbf{i} - (\sinh t) \mathbf{j} + t \mathbf{k} \), describes the curve in 3D space.
  • Compute the first derivative \( \mathbf{r}'(t) = (\sinh t) \mathbf{i} - (\cosh t) \mathbf{j} + \mathbf{k} \). After computing the derivative, you'll notice that it describes the tangent.

Next, the unit tangent vector \( \mathbf{T}(t) \) is determined by normalizing \( \mathbf{r}'(t) \). Normalizing means dividing \( \mathbf{r}'(t) \) by its magnitude. Calculate the magnitude using the formula
  • \( \|\mathbf{r}'(t)\| = \sqrt{(\sinh t)^2 + (\cosh t)^2 + 1^2} \).
  • Using the hyperbolic identity \( \cosh^2 t - \sinh^2 t = 1 \), the magnitude simplifies to \( \sqrt{2} \).
  • Thus, the unit tangent vector is \( \mathbf{T}(t) = \frac{1}{\sqrt{2}}((\sinh t) \mathbf{i} - (\cosh t) \mathbf{j} + \mathbf{k}) \).

Understanding the unit tangent vector helps visualize the path's direction at any given point along the curve.
Curvature
Curvature in differential geometry quantifies how sharply a curve bends at a particular point. A larger curvature means the curve turns more quickly, while a smaller curvature indicates a gentler turn. To find the curvature \( \kappa(t) \) for a space curve like the one considered here, we use the formula
  • \( \kappa(t) = \frac{\|\mathbf{r}''(t) \times \mathbf{r}'(t)\|}{\|\mathbf{r}'(t)\|^3} \).
  • Start by computing the second derivative \( \mathbf{r}''(t) = (\cosh t) \mathbf{i} + (\sinh t) \mathbf{j} \).

Next, find the cross product \( \mathbf{r}''(t) \times \mathbf{r}'(t) \), which gives a vector perpendicular to both derivatives. In this problem, the cross product simplifies substantially
  • The determinant used in the cross product calculation reduces to \( \mathbf{k} \), indicating orthogonality of the resulting vector solely along the \( \mathbf{k} \)-direction.
  • The magnitude \( \|\mathbf{r}''(t) \times \mathbf{r}'(t)\| = 1 \).

Finally, compute the curvature using \( \|\mathbf{r}'(t)\|^3 = (\sqrt{2})^3 = 2\sqrt{2} \). Thus, \( \kappa(t) = \frac{1}{2\sqrt{2}} \), reflecting the curve's bending at each point.
Normal Vector
The normal vector is crucial in understanding the plane in which a curve exists at any given point. It is perpendicular to the unit tangent. To determine the normal vector \( \mathbf{N}(t) \), follow these steps:
  • First, differentiate the unit tangent vector; for this problem, we have \( \mathbf{T}(t) = \frac{1}{\sqrt{2}}(\sinh t \mathbf{i} - \cosh t \mathbf{j} + \mathbf{k}) \).

After differentiating, we find the result
  • \( \mathbf{T}'(t) = \frac{1}{\sqrt{2}}(\cosh t \mathbf{i} + \sinh t \mathbf{j}) \).
  • Here, each component points in the direction of the curve's change.

Next, normalize this derivative to obtain the unit normal vector, ensuring that the length of the vector is consistently 1
  • \( \|\mathbf{T}'(t)\| = 1 \), thus \( \mathbf{N}(t) = \mathbf{T}'(t) = \frac{1}{\sqrt{2}}(\cosh t \mathbf{i} + \sinh t \mathbf{j}) \).

The unit normal vector provides insight into how the curve deviates from the tangent, offering a deeper understanding of its spatial configuration.

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Most popular questions from this chapter

Section 13.4, you found \(\mathbf{T}, \mathbf{N},\) and \(\kappa .\) Now, in the following Exercises 9-16, find \(\mathbf{B}\) and \(\tau\) for these space curves. \(\mathbf{r}(t)=\left(\cos ^{3} t\right) \mathbf{i}+\left(\sin ^{3} t\right) \mathbf{j}, \quad 0< t<\pi / 2\)

\({r}(t)\) is the position of a particle in space at time \(t .\) Find the angle between the velocity and acceleration vectors at time \(t=0 .\) \begin{equation} \mathbf{r}(t)=\left(\frac{\sqrt{2}}{2} t\right) \mathbf{i}+\left(\frac{\sqrt{2}}{2} t-16 t^{2}\right) \mathbf{j} \end{equation}

Ellipse $$ \begin{array}{c}{\text { a. Show that the curve } \mathbf{r}(t)=(\cos t) \mathbf{i}+(\sin t) \mathbf{j}+(1-\cos t) \mathbf{k}} \\ {0 \leq t \leq 2 \pi, \text { is an ellipse by showing that it is the intersection }} \\\ {\text { of a right circular cylinder and a plane. Find equations }} \\\ {\text { for the cylinder and plane. }} \\ {\text { b. Sketch the ellipse on the cylinder. Add to your sketch the unit }} \\ {\text { tangent vectors at } t=0, \pi / 2, \pi, \text { and } 3 \pi / 2 \text { . }}\\\\{\text { c. Show that the acceleration vector always lies parallel to the }} \\ {\text { plane (orthogonal to a vector normal to the plane). Thus, if }} \\ {\text { you draw the acceleration as a vector attached to the ellipse, it }} \\ {\text { will lie in the plane of the ellipse. Add the acceleration vectors }} \\\ {\text { for } t=0, \pi / 2, \pi, \text { and } 3 \pi / 2 \text { to your sketch. }}\\\\{\text { d. Write an integral for the length of the ellipse. Do not try to }} \\ {\text { evaluate the integral; it is nonelementary. }} \\\ {\text { e. Numerical integrator Estimate the length of the ellipse to }} \\\ {\text { two decimal places. }}\end{array} $$

Linear drag Derive the equations $$\begin{aligned} x &=\frac{v_{0}}{k}\left(1-e^{-k l}\right) \cos \alpha \\ y &=\frac{v_{0}}{k}\left(1-e^{-k t}\right)(\sin \alpha)+\frac{g}{k^{2}}\left(1-k t-e^{-k t}\right) \end{aligned}$$ by solving the following initial value problem for a vector \(r\) in the plane. $$ \text{Differential equation:}\frac{d^{2} \mathbf{r}}{d t^{2}}=-g \mathbf{j}-k \mathbf{v}=-g \mathbf{j}-k \frac{d \mathbf{r}}{d t}$$ $$\text{Initial conditions:}\begin{aligned} \mathbf{r}(0) &=\mathbf{0} \\\\\left.\frac{d \mathbf{r}}{d t}\right|_{t=0} &=\mathbf{v}_{0}=\left(v_{0} \cos \alpha\right) \mathbf{i}+\left(\boldsymbol{v}_{0} \sin \alpha\right) \mathbf{j} \end{aligned}$$ The drag coefficient \(k\) is a positive constant representing resistance due to air density, \(v_{0}\) and \(\alpha\) are the projectile's initial speed and launch angle, and \(g\) is the acceleration of gravity.

What can be said about the torsion of a smooth plane curve \(\mathbf{r}(t)=f(t) \mathbf{i}+g(t) \mathbf{j} ?\) Give reasons for your answer.

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