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Arc length approximations Use a calculator to approximate the length of the following curves. In each case, simplify the arc length integral as much as possible before finding an approximation. $$\mathbf{r}(t)=\left\langle t, 4 t^{2}, 10\right\rangle, \text { for }-2 \leq t \leq 2$$

Short Answer

Expert verified
Answer: The approximate length of the curve is 32.349.

Step by step solution

01

Find the derivative of the position vector

To find the derivative of \(\mathbf{r}(t)=\left\langle t, 4 t^{2}, 10\right\rangle\), differentiate each component with respect to t: $$\mathbf{r}'(t)=\left\langle \frac{d}{dt}(t), \frac{d}{dt}(4t^2), \frac{d}{dt}(10)\right\rangle = \left\langle 1, 8t, 0 \right\rangle$$
02

Find the magnitude of the derivative

Now, find the magnitude of the derivative vector \(\mathbf{r}'(t)\): $$||\mathbf{r}'(t)|| = \sqrt{(1)^2 + (8t)^2 + (0)^2} = \sqrt{1 + 64t^2}$$
03

Set up the integral for arc length

The formula for arc length is: $$L = \int_a^b ||\mathbf{r}'(t)|| \, dt$$ In our case, \(a=-2\), \(b=2\), and \(||\mathbf{r}'(t)|| = \sqrt{1 + 64t^2}\). So the integral is $$L = \int_{-2}^2 \sqrt{1 + 64t^2} \, dt$$
04

Approximate the integral using a calculator

Use a calculator to calculate the approximation of the integral: $$L \approx \int_{-2}^2 \sqrt{1 + 64t^2} \, dt \approx 32.349$$ So the approximate length of the curve is 32.349.

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Key Concepts

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

Derivative of Vector Functions
The derivative of a vector function is essentially taking the derivative of each of its components. This concept is critical when investigating the properties of vector curves. In the given exercise, we are presented with a vector function \(\mathbf{r}(t)=\langle t, 4t^2, 10\rangle\). The aim is to find its derivative.

To do this, we differentiate each component with respect to \(t\):
  • First Component: Differentiate \(t\), which gives \(1\).
  • Second Component: Differentiate \(4t^2\), resulting in \(8t\).
  • Third Component: Differentiate the constant \(10\), which gives \(0\).
Thus, the derivative vector is \(\mathbf{r}'(t) = \langle 1, 8t, 0 \rangle\). This derivative helps us understand the change in position along the curve at any point \(t\).

The derivative of the vector function plays a crucial role in determining the motion along a curve and is also a stepping stone toward calculating arc length.
Integral Calculus
Integral calculus provides the tools to compute quantities that involve accumulation, such as the total length, area, or volume. In this exercise, you encounter integral calculus when setting up the arc length integral for evaluation.

The arc length formula involves integrating the magnitude of the derivative vector over the given interval \([-2, 2]\):\[ L = \int_{-2}^2 ||\mathbf{r}'(t)|| \, dt \]Here, calculating the magnitude is a prerequisite step. By converting the problem into an integral of a function over a particular interval, integral calculus allows us to compute continuous sums, which are vital for precise measurement in geometry and physics.

Once simplified, integrals often require numerical methods or calculators to approximate results effectively, as seen when computing arc length in this scenario. Integral calculus not only allows solving for physical quantities like arc length but is foundational in analyzing entire curves.
Length of Curves
The length of a curve is computed using the arc length formula, which integrates the magnitude of the derivative over a specified interval. Understanding this helps us discern how objects move through space and grasp the properties of different trajectories.

In this exercise, to find the length of the curve defined by \(\mathbf{r}(t)=\langle t, 4t^2, 10\rangle\), we first find the derivative and then the magnitude:\[ ||\mathbf{r}'(t)|| = \sqrt{1 + 64t^2} \]We integrate this magnitude between the limits \(-2\) and \(2\):\[ L = \int_{-2}^2 \sqrt{1 + 64t^2} \, dt \]
The result from this integration gives the arc length of the curve. Accurately understanding arc length is essential in geometry and physics, as it directly corresponds to the actual path an object or particle follows in three-dimensional space, marking its trajectory.
Vector Calculus
Vector calculus extends calculus to vector-fields and functions of several variables. It is essential for analyzing physical phenomena across space and time and in diverse fields from engineering to physics.

This exercise is a practical application of vector calculus, where we work with a vector function over time—a position vector \(\mathbf{r}(t)\) describing a path in space. Finding the derivative \(\mathbf{r}'(t)\) gives the velocity vector, and taking the magnitude of this velocity vector helps determine the arc length, an integral part of vector calculus.

The techniques of differentiating and integrating vector functions are foundational in vector calculus, allowing for complex analysis of fields and forces. Problems like these illustrate how vector calculus provides deep insights into the geometry of motion through space.

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Most popular questions from this chapter

Consider an object moving along the circular trajectory \(\mathbf{r}(t)=\langle A \cos \omega t, A \sin \omega t\rangle,\) where \(A\) and \(\omega\) are constants. a. Over what time interval \([0, T]\) does the object traverse the circle once? b. Find the velocity and speed of the object. Is the velocity constant in either direction or magnitude? Is the speed constant? c. Find the acceleration of the object. d. How are the position and velocity related? How are the position and acceleration related? e. Sketch the position, velocity, and acceleration vectors at four different points on the trajectory with \(A=\omega=1\)

A baseball leaves the hand of a pitcher 6 vertical feet above home plate and \(60 \mathrm{ft}\) from home plate. Assume that the coordinate axes are oriented as shown in the figure. a. In the absence of all forces except gravity, assume that a pitch is thrown with an initial velocity of \(\langle 130,0,-3\rangle \mathrm{ft} / \mathrm{s}\) (about \(90 \mathrm{mi} / \mathrm{hr}\) ). How far above the ground is the ball when it crosses home plate and how long does it take for the pitch to arrive? b. What vertical velocity component should the pitcher use so that the pitch crosses home plate exactly \(3 \mathrm{ft}\) above the ground? c. A simple model to describe the curve of a baseball assumes that the spin of the ball produces a constant sideways acceleration (in the \(y\) -direction) of \(c \mathrm{ft} / \mathrm{s}^{2}\). Assume a pitcher throws a curve ball with \(c=8 \mathrm{ft} / \mathrm{s}^{2}\) (one-fourth the acceleration of gravity). How far does the ball move in the \(y\) -direction by the time it reaches home plate, assuming an initial velocity of (130,0,-3) ft/s? d. In part (c), does the ball curve more in the first half of its trip to the plate or in the second half? How does this fact affect the batter? e. Suppose the pitcher releases the ball from an initial position of (0,-3,6) with initial velocity \((130,0,-3) .\) What value of the spin parameter \(c\) is needed to put the ball over home plate passing through the point (60,0,3)\(?\)

An object moves along a straight line from the point \(P(1,2,4)\) to the point \(Q(-6,8,10)\) a. Find a position function \(\mathbf{r}\) that describes the motion if it occurs with a constant speed over the time interval [0,5] b. Find a position function \(\mathbf{r}\) that describes the motion if it occurs with speed \(e^{t}\)

\(\mathbb{R}^{2}\) Consider the vectors \(\mathbf{I}=\langle 1 / \sqrt{2}, 1 / \sqrt{2}\rangle\) and \(\mathbf{J}=\langle-1 / \sqrt{2}, 1 / \sqrt{2}\rangle\). Write the vector \langle 2,-6\rangle in terms of \(\mathbf{I}\) and \(\mathbf{J}\).

Parabolic trajectory In Example 7 it was shown that for the parabolic trajectory \(\mathbf{r}(t)=\left\langle t, t^{2}\right\rangle, \mathbf{a}=\langle 0,2\rangle\) and \(\mathbf{a}=\frac{2}{\sqrt{1+4 t^{2}}}(\mathbf{N}+2 t \mathbf{T}) .\) Show that the second expression for \(\mathbf{a}\) reduces to the first expression.

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