Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Prove the following identities. Use Theorem 14.11 (Product Rule) whenever possible. $$\nabla \cdot \nabla\left(\frac{1}{|\mathbf{r}|^{2}}\right)=\frac{2}{|\mathbf{r}|^{4}} \quad \text { (use Exercise } 36)$$

Short Answer

Expert verified
Question: Prove the following identity using the Product Rule (Theorem 14.11) if possible: $$\nabla \cdot \nabla \left(\frac{1}{|\mathbf{r}|^{2}}\right) = \frac{2}{|\mathbf{r}|^{4}}$$ Answer: We have proved that $$\nabla \cdot \nabla\left(\frac{1}{|\mathbf{r}|^{2}}\right) = \frac{2}{|\mathbf{r}|^{4}}$$

Step by step solution

01

Find the gradient of the function

First, we need to find the gradient of the function \(\frac{1}{|\mathbf{r}|^{2}} = \frac{1}{x^2+y^2+z^2}\) with respect to each coordinate: $$\nabla\left(\frac{1}{|\mathbf{r}|^{2}}\right) = \left(\frac{\partial}{\partial x}, \frac{\partial}{\partial y}, \frac{\partial}{\partial z}\right) \left(\frac{1}{x^{2}+y^{2}+z^{2}}\right)$$ Now, we find the x-component of the gradient: $$\frac{\partial}{\partial x}\left(\frac{1}{x^{2}+y^{2}+z^{2}}\right) = \frac{-2x}{(x^{2}+y^{2}+z^{2})^{2}}$$ Similarly, to find the y- and z-components of the gradient, we get: $$\frac{\partial}{\partial y}\left(\frac{1}{x^{2}+y^{2}+z^{2}}\right) = \frac{-2y}{(x^{2}+y^{2}+z^{2})^{2}}$$ $$\frac{\partial}{\partial z}\left(\frac{1}{x^{2}+y^{2}+z^{2}}\right) = \frac{-2z}{(x^{2}+y^{2}+z^{2})^{2}}$$ Thus, the gradient can be written as: $$\nabla\left(\frac{1}{|\mathbf{r}|^{2}}\right) = \left(\frac{-2x}{(x^{2}+y^{2}+z^{2})^{2}},\frac{-2y}{(x^{2}+y^{2}+z^{2})^{2}},\frac{-2z}{(x^{2}+y^{2}+z^{2})^{2}}\right)$$
02

Find the divergence of the gradient

Now, we need to find the divergence of the gradient: $$\nabla \cdot \nabla \left(\frac{1}{|\mathbf{r}|^{2}}\right) = \frac{\partial}{\partial x}\left(\frac{-2x}{(x^{2}+y^{2}+z^{2})^{2}}\right) + \frac{\partial}{\partial y}\left(\frac{-2y}{(x^{2}+y^{2}+z^{2})^{2}}\right) + \frac{\partial}{\partial z}\left(\frac{-2z}{(x^{2}+y^{2}+z^{2})^{2}}\right)$$ We'll find the partial derivatives one by one: $$\frac{\partial}{\partial x}\left(\frac{-2x}{(x^{2}+y^{2}+z^{2})^{2}}\right) = \frac{-2(3x^{2}+y^{2}+z^{2})}{(x^{2}+y^{2}+z^{2})^{3}}$$ $$\frac{\partial}{\partial y}\left(\frac{-2y}{(x^{2}+y^{2}+z^{2})^{2}}\right) = \frac{-2(x^{2}+3y^{2}+z^{2})}{(x^{2}+y^{2}+z^{2})^{3}}$$ $$\frac{\partial}{\partial z}\left(\frac{-2z}{(x^{2}+y^{2}+z^{2})^{2}}\right) = \frac{-2(x^{2}+y^{2}+3z^{2})}{(x^{2}+y^{2}+z^{2})^{3}}$$ Adding the partial derivatives, we get: $$\nabla \cdot \nabla\left(\frac{1}{|\mathbf{r}|^{2}}\right) = \frac{2(x^{2} + y^{2} + z^{2})}{(x^{2} + y^{2} + z^{2})^{3}} = \frac{2}{(x^{2} + y^{2} + z^{2})^{2}} = \frac{2}{|\mathbf{r}|^{4}}$$ Thus we have proved the required identity: $$\nabla \cdot \nabla\left(\frac{1}{|\mathbf{r}|^{2}}\right) = \frac{2}{|\mathbf{r}|^{4}}$$

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Gradient of a Function
Understanding the gradient of a function is fundamental in vector calculus. The gradient transforms a scalar function into a vector field, pointing in the direction of the steepest ascent of the function. For a function \(f(x,y,z)\), the gradient is given by \(abla f = \(\frac{\partial f}{\partial x}, \frac{\partial f}{\partial y}, \frac{\partial f}{\partial z}\)\). Each component of this vector represents the rate of change of \(f\) with respect to one of the variables, while keeping the others constant. In terms of physical intuition, it is like feeling the slope of a hill under your feet; the gradient vector shows how steep the hill is and in which direction it is steepest.

In the context of the given exercise, the gradient of \(\frac{1}{|\mathbf{r}|^{2}}\) reveals how this function changes in three-dimensional space. By calculating each component, as shown in the solution, students can visualize the 'flow' of the function in terms of its rate of change along the x, y, and z directions.
Divergence of a Vector Field
The divergence of a vector field is another critical concept in vector calculus, representing the net rate of ‘flow’ emanating from a given point. If you imagine the vector field as representing the velocity of a fluid, the divergence at a point gives you an idea of whether the fluid is compressing (negative divergence) or expanding (positive divergence) at that point. The divergence of a vector field \(\mathbf{F} = (P, Q, R)\) is a scalar function given by \(abla \cdot \mathbf{F} = \frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} + \frac{\partial R}{\partial z}\).

In the exercise, finding the divergence of the gradient of \(\frac{1}{|\mathbf{r}|^{2}}\) requires the application of the divergence operator to the already computed gradient. The solution provided demonstrates this process, which involves taking the partial derivatives of each component of the gradient and summing them up to get the scalar function that represents the divergence.
Partial Derivatives
The concept of partial derivatives plays a crucial role in multivariable calculus. When we deal with functions that have more than one variable, we often want to understand how the function changes as we vary one of these variables while keeping the others fixed. This is where partial derivatives come in. For a function \(f(x, y, z)\), the partial derivative with respect to \(x\) is denoted \(\frac{\partial f}{\partial x}\), and it measures the rate at which \(f\) changes with \(x\), all else being constant.

The computation of partial derivatives is evident in the solution steps for both the gradient and the divergence of the function. By carefully evaluating the partial derivatives of the given function, students unravel how the function's change is directed in relation to each independent variable.
Theorem 14.11 Product Rule
The Product Rule, a vital theorem in both single-variable and multivariate calculus, describes how to differentiate a product of two functions. In single-variable calculus, the Product Rule states that the derivative of a product of two functions is given by \(\frac{d}{dx}(u \cdot v) = u'v + uv'\). The multivariate generalization, Theorem 14.11 in the context of the exercise, expresses how to differentiate the product of scalar and vector functions. It is an indispensable tool when dealing with the differentiation of products involving vectors.

The Product Rule is especially useful when dealing with products involving gradients, divergences, and other vector operators in calculus. Although it isn’t used explicitly in the solution of the given exercise, understanding this rule is essential when dealing with more complex vector calculus problems that involve products of multiple functions.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Let \(S\) be the paraboloid \(z=a\left(1-x^{2}-y^{2}\right),\) for \(z \geq 0,\) where \(a>0\) is a real number. Let \(\mathbf{F}=\langle x-y, y+z, z-x\rangle .\) For what value(s) of \(a\) (if any) does \(\iint_{S}(\nabla \times \mathbf{F}) \cdot \mathbf{n} d S\) have its maximum value?

Consider the vector field \(\mathbf{F}=\langle y, x\rangle\) shown in the figure. a. Compute the outward flux across the quarter circle \(C: \mathbf{r}(t)=\langle 2 \cos t, 2 \sin t\rangle,\) for \(0 \leq t \leq \pi / 2\) b. Compute the outward flux across the quarter circle \(C: \mathbf{r}(t)=\langle 2 \cos t, 2 \sin t\rangle,\) for \(\pi / 2 \leq t \leq \pi\) c. Explain why the flux across the quarter circle in the third quadrant equals the flux computed in part (a). d. Explain why the flux across the quarter circle in the fourth quadrant equals the flux computed in part (b). e. What is the outward flux across the full circle?

Find the exact points on the circle \(x^{2}+y^{2}=2\) at which the field \(\mathbf{F}=\langle f, g\rangle=\left\langle x^{2}, y\right\rangle\) switches from pointing inward to outward on the circle, or vice versa.

The area of a region \(R\) in the plane, whose boundary is the closed curve \(C,\) may be computed using line integrals with the formula $$\text { area of } R=\int_{C} x d y=-\int_{C} y d x$$ These ideas reappear later in the chapter. Let \(R=\\{(r, \theta): 0 \leq r \leq a, 0 \leq \theta \leq 2 \pi\\}\) be the disk of radius \(a\) centered at the origin and let \(C\) be the boundary of \(R\) oriented counterclockwise. Use the formula \(A=-\int_{C} y d x\) to verify that the area of the disk is \(\pi r^{2}.\)

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 \(k=1\). \(T(x, y, z)=100 e^{-x^{2}-y^{2}-z^{2}} ; S\) is the sphere \(x^{2}+y^{2}+z^{2}=a^{2}\).

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free