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Find the point on the curve $$\mathbf{r}(t)=(12 \sin t) \mathbf{i}-(12 \cos t) \mathbf{j}+5 t \mathbf{k}$$ at a distance \(13 \pi\) units along the curve from the point (0,-12,0) in the direction opposite to the direction of increasing arc length.

Short Answer

Expert verified
The point is (0, 12, -5\pi).

Step by step solution

01

Find the Arc Length Function

The arc length from a point where a curve is parameterized by \( \mathbf{r}(t) \) is given by the integral \( s(t) = \int_{a}^{t} \vert \mathbf{r}'(u) \vert \, du \). First, find the derivative of \( \mathbf{r}(t) \):\[ \mathbf{r}'(t) = (12 \cos t) \mathbf{i} + (12 \sin t) \mathbf{j} + 5 \mathbf{k} \].The magnitude of \( \mathbf{r}'(t) \) is:\[ \vert \mathbf{r}'(t) \vert = \sqrt{(12 \cos t)^2 + (12 \sin t)^2 + 5^2} = \sqrt{144 + 25} = 13. \]
02

Calculate the Arc Length

Since the magnitude of \( \mathbf{r}'(t) \) is a constant, the arc length from a point \( t=a \) to a point \( t \) is:\[ s(t) = \int_{0}^{t} 13 \, du = 13t. \]
03

Determine the Parameter \( t \)

We are tasked with finding the point at a distance \( 13\pi \) units along the curve from \( t = 0 \), going in the opposite direction. The expression for arc length is given by \( s(t) = 13t \). Thus, we solve \( 13t = -13\pi \) (since we move in the opposite direction):\[ t = -\pi. \]
04

Find the Point \( \mathbf{r}(-\pi) \)

Substitute \( t = -\pi \) into \( \mathbf{r}(t) = (12 \sin t) \mathbf{i} - (12 \cos t) \mathbf{j} + 5t \mathbf{k} \):- \( 12 \sin(-\pi) = 0 \)- \( -12 \cos(-\pi) = 12 \)- \( 5(-\pi) = -5\pi \)Thus, the point is \( (0, 12, -5\pi) \).

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Key Concepts

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

Parametric Equations
Parametric equations are essential when it comes to expressing geometrical shapes and figures in a more flexible manner. A parametric equation represents a curve by using a parameter, often denoted as \( t \).
This allows each point on the curve to be expressed as a vector function of \( t \).
For example, with the vector function \( \mathbf{r}(t) = (12 \sin t) \mathbf{i} - (12 \cos t) \mathbf{j} + 5t \mathbf{k} \), each component corresponds to a different spatial dimension:
  • \( 12 \sin t \) determines the \( x \)-coordinate,

  • \( -12 \cos t \) the \( y \)-coordinate,

  • \( 5t \) the \( z \)-coordinate.
This representation makes it easier to handle complex shapes that cannot be easily described in standard \( x \), \( y \), \( z \) forms.
With these functions, you can analyze various aspects of the curve, such as its path, direction, and rate of change, providing deep insights into the geometric properties.
Vector Calculus
Vector calculus, a fundamental tool in multivariable calculus, plays a crucial role in analyzing vector fields and functions. In this context, vectors are used to describe curves in three-dimensional space.
The curve defined by the parametric equation \( \mathbf{r}(t) \) is a vector-valued function.
To find properties like arc length, we first need to compute the derivative \( \mathbf{r}'(t) \).
This derivative represents the tangent vector to the curve at any point \( t \). For the given vector function, the derivative is:
  • \( \mathbf{r}'(t) = (12 \cos t) \mathbf{i} + (12 \sin t) \mathbf{j} + 5 \mathbf{k} \)
To find the magnitude of the tangent vector, calculate \( \vert \mathbf{r}'(t) \vert \), which is crucial in obtaining the arc length.
This involves taking the square root of the sum of the squares of its components, ultimately leading to an understanding of how fast the curve is being traversed as \( t \) changes.
Vector calculus provides a framework for understanding spatial curves and their dynamics through derivatives and integrals, leading to profound insights about motion and change in three-dimensional space.
Integral Calculus
Integral calculus allows us to compute quantities like the total arc length of a curve from its parametric equations.
The arc length \( s(t) \) from a starting point \( t = a \) to another point along the curve is found through the integral of the magnitude of the derivative:
  • \( s(t) = \int_{a}^{t} \vert \mathbf{r}'(u) \vert \, du \)
For our problem, since \( \vert \mathbf{r}'(t) \vert \) is constant, the arc length simplification becomes simple:
  • \( s(t) = 13t \)
This linear relationship between arc length and \( t \) indicates that for every unit increase in \( t \), the curve progresses 13 units along its path.
To find a specific distance, such as \( 13\pi \), we set up the equation \( 13t = -13\pi \) (to move opposite the arc direction), and solve for \( t = -\pi \).
By evaluating \( \mathbf{r}(-\pi) \), integral calculus lets us locate points along the curve accurately, making it a powerful tool for finding lengths, areas, and volumes in various geometric contexts.

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Most popular questions from this chapter

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: a. Plot the plane curve given in parametric or function form over the specified interval to see what it looks like.b. Calculate the curvature \(\kappa\) of the curve at the given value \(t_{0}\) using the appropriate formula from Exercise 5 or \(6 .\) Use the parametrization \(x=t\) and \(y=f(t)\) if the curve is given as a function \(y=f(x).\)c. Find the unit normal vector \(\mathbf{N}\) at \(t_{0} .\) Notice that the signs of the components of \(\mathbf{N}\) depend on whether the unit tangent vector \(\mathbf{T}\) is turning clockwise or counterclockwise at \(\left.t=t_{0} . \text { (See Exercise } 7 .\right)\) d. If \(\mathbf{C}=a \mathbf{i}+b \mathbf{j}\) is the vector from the origin to the center \((a, b)\) of the osculating circle, find the center \(\mathbf{C}\) from the vector equation $$\mathbf{C}=\mathbf{r}\left(t_{0}\right)+\frac{1}{\kappa\left(t_{0}\right)} \mathbf{N}\left(t_{0}\right),$$ The point \(P\left(x_{0}, y_{0}\right)\) on the curve is given by the position vector \(\mathbf{r}\left(t_{0}\right)\) e. Plot implicitly the equation \((x-a)^{2}+(y-b)^{2}=1 / \kappa^{2}\) of the osculating circle. Then plot the curve and osculating circle together. You may need to experiment with the size of the viewing window, but be sure the axes are equally scaled. $$\mathbf{r}(t)=\left(t^{3}-2 t^{2}-t\right) \mathbf{i}+\frac{3 t}{\sqrt{1+t^{2}}} \mathbf{j}, \quad-2 \leq t \leq 5, \quad t_{0}=1.$$

To illustrate that the length of a smooth space curve does not depend on the parametrization you use to compute it, calculate the length of one turn of the helix in Example 1 with the following parametrizations. a. \(\mathbf{r}(t)=(\cos 4 t) \mathbf{i}+(\sin 4 t) \mathbf{j}+4 t \mathbf{k}, \quad 0 \leq t \leq \pi / 2\) b. \(\mathbf{r}(t)=[\cos (t / 2)] \mathbf{i}+[\sin (t / 2)] \mathbf{j}+(t / 2) \mathbf{k}, \quad 0 \leq t \leq 4 \pi\) c. \(\mathbf{r}(t)=(\cos t) \mathbf{i}-(\sin t) \mathbf{j}-t \mathbf{k}, \quad-2 \pi \leq t \leq 0\)

a. Use Corollary 2 of the Mean Value Theorem for scalar functions to show that if two vector functions \(\mathbf{R}_{1}(t)\) and \(\mathbf{R}_{2}(t)\) have identical derivatives on an interval \(I\), then the functions differ by a constant vector value throughout \(I\) b. Use the result in part (a) to show that if \(\mathbf{R}(t)\) is any antiderivative of \(\mathbf{r}(t)\) on \(I\), then any other antiderivative of \(\mathbf{r}\) on \(I\) equals \(\mathbf{R}(t)+\mathbf{C}\) for some constant vector \(\mathbf{C}\)

Show that \(\kappa\) and \(\tau\) are both zero for the line \(\mathbf{r}(t)=\left(x_{0}+A t\right) \mathbf{i}+\left(y_{0}+B t\right) \mathbf{j}+\left(z_{0}+C t\right) \mathbf{k}\).

A baseball is hit when it is \(0.8 \mathrm{m}\) above the ground. It leaves the bat with an initial velocity of \(40 \mathrm{m} / \mathrm{s}\) 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 \(-4 \mathbf{i}(\mathrm{m} / \mathrm{s})\) to the ball's initial velocity. \(\mathrm{A}\) 5-m-high fence lies \(90 \mathrm{m}\) 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 6 m high? How far (ground distance) is the baseball from home plate at that height? e. Has the batter hit a home run? Explain.

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