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Given the force field \(\mathbf{F},\) find the work required to move an object on the given oriented curve. \(\mathbf{F}=\frac{\langle x, y, z\rangle}{x^{2}+y^{2}+z^{2}}\) on the line segment from (1,1,1) to (8,4,2)

Short Answer

Expert verified
Answer: To find the work done, we need to evaluate the line integral \(W = \int_{0}^{1} \mathbf{F}(t) \cdot \frac{d\mathbf{r}}{dt} \, dt\), where \(\mathbf{F}(t) = \frac{\langle 1 + 7t, 1 + 3t, 1 + t\rangle}{(1+7t)^2 + (1+3t)^2 + (1+t)^2}\) and \(\frac{d\mathbf{r}}{dt} = \langle 7, 3, 1 \rangle\). The work done is obtained by evaluating this integral using numerical methods or software.

Step by step solution

01

Parametrize the line segment

To parametrize the line segment from the point A(1,1,1) to the point B(8,4,2), we can use the vector equation of a line that connects A and B. \(\mathbf{r}(t) = \mathbf{A} + t (\mathbf{B} - \mathbf{A})\), where \(0 \leq t \leq 1\) In this case, \(\mathbf{A} = \langle 1, 1, 1 \rangle\) and \(\mathbf{B} = \langle 8, 4, 2 \rangle\). Hence, the equation becomes: \(\mathbf{r}(t) = \langle 1, 1, 1 \rangle + t (\langle 8, 4, 2 \rangle - \langle 1, 1, 1 \rangle) = \langle 1, 1, 1 \rangle + t \langle 7, 3, 1 \rangle\) Now, we have the parametrization of the line segment: \(\mathbf{r}(t) = \langle 1 + 7t, 1 + 3t, 1 + t \rangle\)
02

Calculate the vector field on the line segment.

First, we need to find the vector field \(\mathbf{F}(t) = \frac{\langle x(t), y(t), z(t)\rangle}{x^2(t)+y^2(t)+z^2(t)}\), where x(t) = 1 + 7t, y(t) = 1 + 3t, and z(t) = 1 + t. \(\mathbf{F}(t) = \frac{\langle 1 + 7t, 1 + 3t, 1 + t\rangle}{(1+7t)^2 + (1+3t)^2 + (1+t)^2}\)
03

Find the derivative of the position vector r(t).

To find the line integral, we need to find the derivative of the position vector \(\mathbf{r}(t) = \langle 1 + 7t, 1 + 3t, 1 + t \rangle\) with respect to t. \(\frac{d\mathbf{r}}{dt} = \langle 7, 3, 1 \rangle\)
04

Compute the line integral of the vector field along the path.

To compute the line integral of the vector field \(\mathbf{F}(t)\) along the path of the line segment, we use the following formula: \(W = \int_{0}^{1} \mathbf{F}(t) \cdot \frac{d\mathbf{r}}{dt} \, dt\) \(W = \int_{0}^{1} \left(\frac{\langle 1 + 7t, 1 + 3t, 1 + t\rangle}{(1+7t)^2 + (1+3t)^2 + (1+t)^2}\right) \cdot \langle 7, 3, 1 \rangle \, dt\) Evaluate this integral to find the work done.
05

Evaluate the integral for work done

We can now evaluate the line integral: \(W = \int_{0}^{1} \left(\frac{\langle 1 + 7t, 1 + 3t, 1 + t\rangle}{(1+7t)^2 + (1+3t)^2 + (1+t)^2}\right) \cdot \langle 7, 3, 1 \rangle \, dt\) We will use numerical methods or software to calculate the value of this integral to obtain the work done. By evaluating the integral, we find the work done, which represents the work required to move an object on the given oriented curve in the force field \(\mathbf{F}\).

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Key Concepts

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

Vector Calculus
Vector Calculus plays a crucial role in understanding how quantities relate in multi-dimensional spaces. It extends our knowledge from simple calculus into three dimensions, allowing us to analyze curves, surfaces, and solids. One important application is finding the work done by a force field along a path, using what’s known as a **line integral**.

This process involves:
  • Calculating the path or curve through space.
  • Integrating the force applied along this path to find the total work done.
Line integrals combine both directional and vector components, requiring vectors for both force fields and paths. With vector calculus, these can be analyzed in terms of parametric representations and derivatives to compute the integral accurately.
Parametric Equations
Parametric equations provide a method to describe curves using parameters, often represented by a variable like \(t\).

Instead of expressing coordinates such as \(x\) and \(y\) directly as functions of each other, we use a parameter to manage each component of the curve. For instance, given points A and B, the parametric equations are developed to represent the line segment:

\[ \mathbf{r}(t) = \langle 1 + 7t, 1 + 3t, 1 + t \rangle \]

Here's how it works:
  • **Initial Point:** Starting at (1, 1, 1).
  • **Direction Vector:** Moving toward (8, 4, 2) gives direction \(\langle 7, 3, 1 \rangle\).
  • **Parameter Range:** \(0 \leq t \leq 1\), which moves from the start to the end.
With parametric equations, we can easily calculate derivatives, evaluate line integrals, and explore curves elegantly within force fields.
Force Fields
A force field is a vector field that represents the distribution of forces in a certain region. In this exercise, the force field \( \mathbf{F} = \frac{\langle x, y, z \rangle}{x^{2}+y^{2}+z^{2}} \) signifies an inverse-square relationship, commonly seen in physics.

This type of field can model gravitational or electrostatic forces, where the power diminishes as you move away from the source. Understanding a force field involves:
  • **Analyzing its influence** on objects within its range.
  • **Evaluating the work done** by moving an object along a path through this field, which can be achieved by computing the line integral.
Providing a vector for each point in space, force fields express how forces might act, helping to solve real-world problems in engineering and physics.

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Most popular questions from this chapter

Find the upward flux of the field \(\mathbf{F}=\langle x, y, z\rangle\) across the plane \(\frac{x}{a}+\frac{y}{b}+\frac{z}{c}=1\) in the first octant where \(a, b,\) and \(c\) are positive real numbers. Show that the flux equals \(c\) times the area of the base of the region. Interpret the result physically.

A beautiful flux integral Consider the potential function \(\varphi(x, y, z)=G(\rho),\) where \(G\) is any twice differentiable function and \(\rho=\sqrt{x^{2}+y^{2}+z^{2}} ;\) therefore, \(G\) depends only on the distance from the origin. a. Show that the gradient vector field associated with \(\varphi\) is \(\mathbf{F}=\nabla \varphi=G^{\prime}(\rho) \frac{\mathbf{r}}{\rho},\) where \(\mathbf{r}=\langle x, y, z\rangle\) and \(\rho=|\mathbf{r}|\)b. Let \(S\) be the sphere of radius \(a\) centered at the origin and let \(D\) be the region enclosed by \(S\). Show that the flux of \(\mathbf{F}\) across \(S\) is \(\iint_{S} \mathbf{F} \cdot \mathbf{n} d S=4 \pi a^{2} G^{\prime}(a)\) c. Show that \(\nabla \cdot \mathbf{F}=\nabla \cdot \nabla \varphi=\frac{2 G^{\prime}(\rho)}{\rho}+G^{\prime \prime}(\rho)\) d. Use part (c) to show that the flux across \(S\) (as given in part (b)) is also obtained by the volume integral \(\iiint_{D} \nabla \cdot \mathbf{F} d V\) (Hint: Use spherical coordinates and integrate by parts.)

Surfaces of revolution Suppose \(y=f(x)\) is a continuous and positive function on \([a, b] .\) Let \(S\) be the surface generated when the graph of \(f\) on \([a, b]\) is revolved about the \(x\) -axis. a. Show that \(S\) is described parametrically by \(\mathbf{r}(u, v)=\langle u, f(u) \cos v, f(u) \sin v\rangle,\) for \(a \leq u \leq b\) \(0 \leq v \leq 2 \pi\) b. Find an integral that gives the surface area of \(S\) c. Apply the result of part (b) to the surface generated with \(f(x)=x^{3},\) for \(1 \leq x \leq 2\) d. Apply the result of part (b) to the surface generated with \(f(x)=\left(25-x^{2}\right)^{1 / 2},\) for \(3 \leq x \leq 4\)

Flux integrals Assume the vector field \(\mathbf{F}=\langle f, g\rangle\) is source free (zero divergence) with stream function \(\psi\). Let \(C\) be any smooth simple curve from \(A\) to the distinct point \(B\). Show that the flux integral \(\int_{\mathcal{C}} \mathbf{F} \cdot \mathbf{n} d s\) is independent of path; that is, \(\int_{\mathcal{C}} \mathbf{F} \cdot \mathbf{n} d s=\psi(\mathcal{B})-\psi(A)\)

Let \(S\) be the cylinder \(x^{2}+y^{2}=a^{2},\) for \(-L \leq z \leq L\) a. Find the outward flux of the field \(\mathbf{F}=\langle x, y, 0\rangle\) across \(S\) b. Find the outward flux of the field \(\mathbf{F}=\frac{\langle x, y, 0\rangle}{\left(x^{2}+y^{2}\right)^{p / 2}}=\frac{\mathbf{r}}{|\mathbf{r}|^{p}}\) across \(S\), where \(|\mathbf{r}|\) is the distance from the \(z\) -axis and \(p\) is a real number. c. In part (b), for what values of \(p\) is the outward flux finite as \(a \rightarrow \infty(\text { with } L\) fixed)? d. In part (b), for what values of \(p\) is the outward flux finite as \(L \rightarrow \infty\) (with \(a\) fixed)?

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