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Prove that for a real number \(p,\) with \(\mathbf{r}=\langle x, y, z\rangle, \nabla\left(\frac{1}{|\mathbf{r}|^{p}}\right)=\frac{-p \mathbf{r}}{|\mathbf{r}|^{p+2}}.\)

Short Answer

Expert verified
Given a vector 饾惈=鉄▁, y, z鉄 and a function f(饾惈)=1/|饾惈|^p, prove the identity that the gradient of the function is equal to -p饾惈/|饾惈|^(p+2). Answer: Using the chain rule, we calculated the gradient of the function f(饾惈) and found it to be: 鈭噁(饾惈) = 鉄-px/|饾惈|^(p+2), -py/|饾惈|^(p+2), -pz/|饾惈|^(p+2)鉄 = -p饾惈/|饾惈|^(p+2) Thus, the gradient of the function f(饾惈)=1/|饾惈|^p is indeed equal to -p饾惈/|饾惈|^(p+2).

Step by step solution

01

Write down the function to work with in terms of x, y, and z

Given the vector \(\mathbf{r}=\langle x, y, z\rangle\), we can define the function \(f(\mathbf{r})\) as \(f(\mathbf{r})=\frac{1}{|\mathbf{r}|^p}\), where \(|\mathbf{r}|=\sqrt{x^2+y^2+z^2}\).
02

Determine the gradient of the function

The gradient of the function is a vector given by the partial derivatives of the function with respect to each coordinate: $$ \nabla f(\mathbf{r}) = \left\langle\frac{\partial f}{\partial x}, \frac{\partial f}{\partial y}, \frac{\partial f}{\partial z}\right\rangle $$
03

Calculate the partial derivatives

We can use the Chain Rule to determine the partial derivatives: $$ \frac{\partial f}{\partial x} = \frac{\mathrm{d}f}{\mathrm{d}|\mathbf{r}|} \frac{\partial|\mathbf{r}|}{\partial x} $$ First, we will find the derivative of \(f\) with respect to \(|\mathbf{r}|\): $$ \frac{\mathrm{d}f}{\mathrm{d}|\mathbf{r}|} = \frac{\mathrm{d}}{\mathrm{d}|\mathbf{r}|}\left(\frac{1}{|\mathbf{r}|^p}\right) = \frac{-p}{|\mathbf{r}|^{p+1}} $$ For the derivative of \(|\mathbf{r}|\) with respect to each coordinate, we can differentiate the expression for \(|\mathbf{r}|=\sqrt{x^2+y^2+z^2}\): $$ \frac{\partial |\mathbf{r}|}{\partial x} = \frac{x}{|\mathbf{r}|} $$ Using the Chain Rule, we obtain the partial derivative of \(f\) with respect to \(x\): $$ \frac{\partial f}{\partial x} = \frac{-p}{|\mathbf{r}|^{p+1}} \cdot \frac{x}{|\mathbf{r}|} = \frac{-px}{|\mathbf{r}|^{p+2}} $$ Similarly, we find the partial derivatives with respect to \(y\) and \(z\): $$ \frac{\partial f}{\partial y} = \frac{-py}{|\mathbf{r}|^{p+2}} $$ $$ \frac{\partial f}{\partial z} = \frac{-pz}{|\mathbf{r}|^{p+2}} $$
04

Form the gradient

Now that we have all the partial derivatives, we can form the gradient of \(f(\mathbf{r})\): $$ \nabla f(\mathbf{r}) = \left\langle \frac{-px}{|\mathbf{r}|^{p+2}}, \frac{-py}{|\mathbf{r}|^{p+2}}, \frac{-pz}{|\mathbf{r}|^{p+2}} \right\rangle = \frac{-p\mathbf{r}}{|\mathbf{r}|^{p+2}} $$ This completes the proof that \(\nabla\left(\frac{1}{|\mathbf{r}|^p}\right) = \frac{-p\mathbf{r}}{|\mathbf{r}|^{p+2}}\).

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Key Concepts

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

Vector Calculus
Vector calculus is a branch of mathematics concerned with differentiation and integration of vector fields. It extends the concepts of calculus to functions of several variables, often producing results that are vectors themselves. In this context, the gradient is a crucial vector concept. It gives the direction of the steepest ascent of a scalar field, indicating how a function changes at a particular point in space.
To visualize, imagine temperature at different points in a room. The gradient vector at any point would show the direction in which the temperature rises fastest.
In the given exercise, the vector \(\mathbf{r}=\langle x, y, z \rangle\) represents a position in three-dimensional space. The operation \(abla\left(\frac{1}{|\mathbf{r}|^p}\right)\) involves calculating the gradient - a key part of vector calculus.
Partial Derivatives
Partial derivatives measure how a function changes as one of its variables is varied while keeping others constant. If you think of a multivariable function as a landscape, partial derivatives tell you the slope in specific directions.
In simpler terms, while calculating partial derivatives of a function like \(f(x, y, z) = \frac{1}{|\mathbf{r}|^p}\), you're assessing how the function value changes with respect to each individual variable: \(x, y, \) and \(z\).
These calculations are foundational in determining the gradient. For the function in question, we differentiate with respect to \(x, y,\) and \(z\), keeping the others constant at one step.
Thus, even though only the "x" variable might change during one partial differentiation, the effects of "y" and "z" remain frozen as constants. This process helps us form a complete gradient vector solution.
Chain Rule
The Chain Rule is an essential tool in calculus used to differentiate composite functions. It combines derivatives of separate functions in nested situations. To put it plainly, it helps find out how a change in one variable passes through several layers of functions, resulting in a change in the final outcome.
In the exercise, the Chain Rule is utilized to compute the partial derivatives of the function \(f(\mathbf{r}) = \frac{1}{|\mathbf{r}|^p}\). When calculating \(\frac{\partial f}{\partial x}\), first, the inner derivative \(\frac{\mathrm{d}f}{\mathrm{d}|\mathbf{r}|}\) is computed. Then, it is multiplied by the outer derivative \(\frac{\partial|\mathbf{r}|}{\partial x}\).
This two-stage approach is repeated for each variable \(x, y, \) and \(z\) to form the components of the gradient vector. By chaining together these derivatives, we can effectively tackle more complex multivariable functions and how they interact with one another.

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Most popular questions from this chapter

Consider the radial vector fields \(\mathbf{F}=\mathbf{r} /|\mathbf{r}|^{p},\) where \(p\) is a real number and \(\mathbf{r}=\langle x, y, z\rangle\) Let \(C\) be any circle in the \(x y\) -plane centered at the origin. a. Evaluate a line integral to show that the field has zero circulation on \(C\) b. For what values of \(p\) does Stokes' Theorem apply? For those values of \(p,\) use the surface integral in Stokes' Theorem to show that the field has zero circulation on \(C\).

The heat flow vector field for conducting objects is \(\mathbf{F}=-k \nabla T,\) where \(T(x, y, z)\) is the temperature in the object and \(k>0\) is a constant that depends on the material. Compute the outward flux of \(\mathbf{F}\) across the following surfaces S for the given temperature distributions. Assume \(k=1\). \(T(x, y, z)=100 e^{-x-y} ; S\) consists of the faces of the cube \(|x| \leq 1,|y| \leq 1,|z| \leq 1\).

A square plate \(R=\\{(x, y): 0 \leq x \leq 1,\) \(0 \leq y \leq 1\\}\) has a temperature distribution \(T(x, y)=100-50 x-25 y\) a. Sketch two level curves of the temperature in the plate. b. Find the gradient of the temperature \(\nabla T(x, y)\) c. Assume that the flow of heat is given by the vector field \(\mathbf{F}=-\nabla T(x, y) .\) Compute \(\mathbf{F}\) d. Find the outward heat flux across the boundary \(\\{(x, y): x=1,0 \leq y \leq 1\\}\) e. Find the outward heat flux across the boundary \(\\{(x, y): 0 \leq x \leq 1, y=1\\}\)

Let \(f\) be differentiable and positive on the interval \([a, b] .\) Let \(S\) be the surface generated when the graph of \(f\) on \([a, b]\) is revolved about the \(x\) -axis. Use Theorem 14.12 to show that the area of \(S\) (as given in Section 6.6 ) is $$ \int_{a}^{b} 2 \pi f(x) \sqrt{1+f^{\prime}(x)^{2}} d x $$.

Prove that for a real number \(p\), with \(\mathbf{r}=\langle x, y, z\rangle, \nabla \cdot \nabla\left(\frac{1}{|\mathbf{r}|^{p}}\right)=\frac{p(p-1)}{|\mathbf{r}|^{p+2}}.\)

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