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Find the curvature and the radius of curvature at the stated point. $$ \mathbf{r}(t)=3 \cos t \mathbf{i}+4 \sin t \mathbf{j}+t \mathbf{k} ; \quad t=\pi / 2 $$

Short Answer

Expert verified
Curvature is \( \frac{2}{5} \) and the radius of curvature is \( \frac{5}{2} \).

Step by step solution

01

Find the first derivative

To find the curvature, begin by determining the velocity vector, which is the first derivative of the position vector \( \mathbf{r}(t) \) with respect to \( t \). The derivative is: \[ \mathbf{r}'(t) = \frac{d}{dt}(3 \cos t) \mathbf{i} + \frac{d}{dt}(4 \sin t) \mathbf{j} + \frac{d}{dt} t \mathbf{k} = -3 \sin t \mathbf{i} + 4 \cos t \mathbf{j} + \mathbf{k} \]
02

Find the second derivative

Next, find the acceleration vector, which is the second derivative of \( \mathbf{r}(t) \). Differentiate \( \mathbf{r}'(t) \) with respect to \( t \).\[ \mathbf{r}''(t) = \frac{d}{dt}(-3 \sin t) \mathbf{i} + \frac{d}{dt}(4 \cos t) \mathbf{j} + \frac{d}{dt}(1) \mathbf{k} = -3 \cos t \mathbf{i} - 4 \sin t \mathbf{j} \]
03

Evaluate the vectors at the given parameter

Substitute \( t = \frac{\pi}{2} \) into \( \mathbf{r}'(t) \) and \( \mathbf{r}''(t) \):\[ \mathbf{r}'\left(\frac{\pi}{2}\right) = -3 \sin\left(\frac{\pi}{2}\right) \mathbf{i} + 4 \cos\left(\frac{\pi}{2}\right) \mathbf{j} + \mathbf{k} = -3 \mathbf{i} + \mathbf{k} \]\[ \mathbf{r}''\left(\frac{\pi}{2}\right) = -3 \cos\left(\frac{\pi}{2}\right) \mathbf{i} - 4 \sin\left(\frac{\pi}{2}\right) \mathbf{j} = -4 \mathbf{j} \]
04

Calculate the cross product

Use the evaluated vectors to compute the cross product \( \mathbf{r}'\left(\frac{\pi}{2}\right) \times \mathbf{r}''\left(\frac{\pi}{2}\right) \):\[ \mathbf{r}'\left(\frac{\pi}{2}\right) \times \mathbf{r}''\left(\frac{\pi}{2}\right) = (-3 \mathbf{i} + \mathbf{k}) \times (-4 \mathbf{j}) = 12 \mathbf{k} + 4 \mathbf{i} \]
05

Determine the magnitudes

Calculate the magnitudes of \( \mathbf{r}'\left(\frac{\pi}{2}\right) \) and \( \mathbf{r}'\left(\frac{\pi}{2}\right) \times \mathbf{r}''\left(\frac{\pi}{2}\right) \):\[ \left\| \mathbf{r}'\left(\frac{\pi}{2}\right) \right\| = \sqrt{(-3)^2 + (0)^2 + (1)^2} = \sqrt{10} \]\[ \left\| \mathbf{r}'\left(\frac{\pi}{2}\right) \times \mathbf{r}''\left(\frac{\pi}{2}\right) \right\| = \sqrt{(4)^2 + (0)^2 + (12)^2} = \sqrt{160} = 4\sqrt{10} \]
06

Compute the curvature and radius of curvature

The curvature \( \kappa \) is given by:\[ \kappa = \frac{\left\| \mathbf{r}' \times \mathbf{r}'' \right\|}{\left\| \mathbf{r}' \right\|^3} = \frac{4\sqrt{10}}{(\sqrt{10})^3} = \frac{4\sqrt{10}}{10\sqrt{10}} = \frac{2}{5} \]The radius of curvature \( R \) is the reciprocal of the curvature:\[ R = \frac{1}{\kappa} = \frac{5}{2} \]
07

Conclude the result

At \( t = \frac{\pi}{2} \), the curvature is \( \frac{2}{5} \) and the radius of curvature is \( \frac{5}{2} \).

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Key Concepts

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

Velocity Vector
The velocity vector is a fundamental concept in calculus and physics. It describes the direction and speed of a moving object at a particular point in time.

To find it, you take the derivative of the position vector, which represents the path of the object. In the exercise, the position vector is given by \( \mathbf{r}(t) = 3 \cos t \mathbf{i} + 4 \sin t \mathbf{j} + t \mathbf{k} \).

The derivative of this position vector gives us the velocity vector: \( \mathbf{r}'(t) = -3 \sin t \mathbf{i} + 4 \cos t \mathbf{j} + \mathbf{k} \).

This vector tells us how fast the object is moving in the direction of each axis (i, j, k). Specifically, it shows changes over time, such as \(-3 \sin t\) along the i-axis, \(4 \cos t\) along the j-axis, and a constant speed along the k-axis.
Acceleration Vector
The acceleration vector is the next derivative after the velocity vector. It tells us how the velocity of an object changes over time. To find it, we take the derivative of the velocity vector.

In our task, this is done by differentiating the velocity \( \mathbf{r}'(t) \) which yields the acceleration vector \( \mathbf{r}''(t) = -3 \cos t \mathbf{i} - 4 \sin t \mathbf{j} \).

This vector indicates how quickly the velocity is changing along each axis. An important thing to note is that unlike the velocity vector, the acceleration vector does not have a component in the k-direction, meaning the speed in that direction is not changing.
Cross Product
The cross product is a mathematical operation that takes two vectors and returns another vector perpendicular to the plane of the first two. It has applications in calculating the curvature and can be visualized as the area of a parallelogram formed by the two vectors.

In our exercise, the cross product is used to help determine the curvature. We compute it from the evaluated velocity and acceleration vectors:

\( \mathbf{r}'\left(\frac{\pi}{2}\right) = -3 \mathbf{i} + \mathbf{k} \) and \( \mathbf{r}''\left(\frac{\pi}{2}\right) = -4 \mathbf{j} \). The resulting cross product is \( 12 \mathbf{k} + 4 \mathbf{i} \), which represents a vector perpendicular to both these vectors.
Radius of Curvature
The radius of curvature gives information about the "bendiness" or sharpness of a curve at a given point.

Mathematically, it is often the reciprocal of curvature. While curvature measures how quickly a curve changes direction, the radius of curvature quantifies how large or small the circle would be that "fits" the curve at that point.

In the problem, once the curvature \( \kappa \) is calculated as \( \frac{2}{5} \), the radius of curvature \( R \) is simply the reciprocal: \( \frac{5}{2} \).

This indicates how gentle or tight the path is turning at \( t = \frac{\pi}{2} \), offering a geometrical perspective on the trajectory's behavior at that moment.

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Most popular questions from this chapter

Use the given information to find the normal scalar component of acceleration at time \(t=1\). $$ \mathbf{a}(1)=\mathbf{i}+2 \mathbf{j}-2 \mathbf{k} ; a_{T}(1)=3 $$

A shell is fired from ground level at an elevation angle of \(\alpha\) and a muzzle speed of \(\underline{v_{0} \text { . }}\) (a) Show that the maximum height reached by the shell is $$ \text { maximum height }=\frac{\left(v_{0} \sin \alpha\right)^{2}}{2 g} $$ (b) The horizontal range \(R\) of the shell is the horizontal distance traveled when the shell returns to ground level. Show that \(R=\left(v_{0}^{2} \sin 2 \alpha\right) / g .\) For what elevation angle will the range be maximum? What is the maximum range?

Use the given information to find the normal scalar component of acceleration at time \(t=1\) $$ \|\mathbf{a}(1)\|=9 ; a_{T}(1) \mathbf{T}(1)=2 \mathbf{i}-2 \mathbf{j}+\mathbf{k} $$

Let \(\mathbf{r}(t)=t^{2} \mathbf{i}+t^{3} \mathbf{j}\) (see Figure 12.3.1). Let \(\theta(t)\) be the angle between \(\mathbf{r}^{\prime}(t)\) and \(\mathbf{i}\). Show that $$ \theta(t) \rightarrow \pi \text { as } t \rightarrow 0^{-} \quad \text { and } \quad \theta(t) \rightarrow 0 \text { as } t \rightarrow 0^{+} $$

(a) Find the arc length parametrization of the line $$ x=-5+3 t, \quad y=2 t, \quad z=5+t $$ that has the same direction as the given line and has reference point \((-5,0,5)\). (b) Use the parametric equations obtained in part (a) to find the point on the line that is 10 units from the reference point in the direction of increasing parameter.

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