Chapter 14: Problem 77
Verify that the function \(u=1 / \sqrt{x^{2}+y^{2}+z^{2}}\) is a solution of the three-dimensional Laplace equation \(u_{x x}+u_{y y}+u_{z z}=0\)
Short Answer
Expert verified
The function satisfies the Laplace equation, so it is a solution.
Step by step solution
01
Compute Partial Derivatives
Given the function \[ u = \frac{1}{\sqrt{x^2 + y^2 + z^2}}.\]First, express it as \( u = (x^2 + y^2 + z^2)^{-1/2} \). Now compute the first-order partial derivatives using the chain rule. For \( u_x \), differentiate with respect to \( x \):\[ u_x = -(x^2 + y^2 + z^2)^{-3/2} \cdot x.\]Similarly, compute for \( u_y \) and \( u_z \):\[u_y = -(x^2 + y^2 + z^2)^{-3/2} \cdot y,\]\[u_z = -(x^2 + y^2 + z^2)^{-3/2} \cdot z.\]
02
Compute Second-Order Partial Derivatives
Now compute the second-order partial derivatives. For \( u_{xx} \), apply the product rule to \( u_x \):\[ u_{xx} = \frac{\partial}{\partial x} \left( -(x^2 + y^2 + z^2)^{-3/2} \cdot x \right).\]This yields:\[u_{xx} = (x^2 + y^2 + z^2)^{-5/2} (2x^2 - y^2 - z^2).\]Similarly, compute \( u_{yy} \) and \( u_{zz} \):\[u_{yy} = (x^2 + y^2 + z^2)^{-5/2} (2y^2 - x^2 - z^2),\]\[u_{zz} = (x^2 + y^2 + z^2)^{-5/2} (2z^2 - x^2 - y^2).\]
03
Verify Laplace's Equation
Now, substitute the second-order derivatives into Laplace’s equation \[ u_{xx} + u_{yy} + u_{zz} = 0. \]Substitute the expressions from Step 2:\[(x^2 + y^2 + z^2)^{-5/2} (2x^2 - y^2 - z^2) + (x^2 + y^2 + z^2)^{-5/2} (2y^2 - x^2 - z^2) + (x^2 + y^2 + z^2)^{-5/2} (2z^2 - x^2 - y^2)= 0.\]Simplify the equation by combining terms:\[(x^2 + y^2 + z^2)^{-5/2} (2x^2 + 2y^2 + 2z^2 - (x^2 + y^2 + z^2)) = 0,\]which simplifies to:\[(x^2 + y^2 + z^2)^{-5/2} \cdot 0 = 0.\]Hence, the function satisfies Laplace's equation.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Partial Derivatives
Partial derivatives are a fundamental concept in calculus, especially when dealing with functions of several variables. When we have a multivariable function, like in our exercise with variables \(x\), \(y\), and \(z\), each variable might influence the outcome independently. A partial derivative of a function is its derivative with respect to one of these variables, treating all the other variables as constant.
For the given function \(u = \frac{1}{\sqrt{x^2 + y^2 + z^2}}\), the partial derivative with respect to \(x\) is taken by differentiating \(u\) with \(x\) while keeping \(y\) and \(z\) constant, resulting in:
Partial derivatives are crucial when checking if a function satisfies differential equations, such as the Laplace equation, by showing changes with respect to each variable separately.
For the given function \(u = \frac{1}{\sqrt{x^2 + y^2 + z^2}}\), the partial derivative with respect to \(x\) is taken by differentiating \(u\) with \(x\) while keeping \(y\) and \(z\) constant, resulting in:
- \(u_x = -(x^2 + y^2 + z^2)^{-3/2} \cdot x\)
Partial derivatives are crucial when checking if a function satisfies differential equations, such as the Laplace equation, by showing changes with respect to each variable separately.
Three-Dimensional Calculus
Three-dimensional calculus extends calculus to three-dimensional space, involving functions with three variables. It's highly applicable in physics and engineering, where many processes occur in three dimensions. In our problem, we deal with a potential field represented by the function \(u = \frac{1}{\sqrt{x^2 + y^2 + z^2}}\), which is a common representation in electrostatics and fluid dynamics.
To explore functions in three dimensions, we use tools such as gradients, divergence, and Laplacians. The Laplace equation, \(u_{xx} + u_{yy} + u_{zz} = 0\), is especially important in finding scalar potentials where equilibrium conditions hold, meaning there's no change in potential in any direction. Thus, checking each second-order partial derivative implies exploring how the function changes shape or size when moving along the \(x\), \(y\), and \(z\) axes.
By confirming \(u_{xx} + u_{yy} + u_{zz} = 0\), we affirm that the function `u` represents a harmonic function, important when solving real-world physics problems involving three dimensions.
To explore functions in three dimensions, we use tools such as gradients, divergence, and Laplacians. The Laplace equation, \(u_{xx} + u_{yy} + u_{zz} = 0\), is especially important in finding scalar potentials where equilibrium conditions hold, meaning there's no change in potential in any direction. Thus, checking each second-order partial derivative implies exploring how the function changes shape or size when moving along the \(x\), \(y\), and \(z\) axes.
By confirming \(u_{xx} + u_{yy} + u_{zz} = 0\), we affirm that the function `u` represents a harmonic function, important when solving real-world physics problems involving three dimensions.
Chain Rule
The chain rule is a powerful tool in calculus used for differentiating composite functions. It allows us to differentiate functions nested within other functions by following a simple principle: differentiate the outer function and then multiply by the derivative of the inner function.
In the given exercise, our function is expressed as \(u = (x^2 + y^2 + z^2)^{-1/2}\). To find \(u_x\), \(u_y\), and \(u_z\), the chain rule assists in handling the exponentiation and square root operations.
In the given exercise, our function is expressed as \(u = (x^2 + y^2 + z^2)^{-1/2}\). To find \(u_x\), \(u_y\), and \(u_z\), the chain rule assists in handling the exponentiation and square root operations.
- First, differentiate \((x^2 + y^2 + z^2)^{-1/2}\) as if it were a simple power function, \(-1/2 (x^2 + y^2 + z^2)^{-3/2}\).
- Then multiply by the derivative of the inner function, \(2x\) for \(x\), \(2y\) for \(y\), and \(2z\) for \(z\).