Chapter 4: Problem 23
$$\text { If } u=f(x-c t)+g(x+c t), \text { show that } \frac{\partial^{2} u}{\partial x^{2}}=\frac{1}{c^{2}} \frac{\partial^{2} u}{\partial t^{2}}$$.
Short Answer
Expert verified
We showed that \( \frac{\text{d}^2 u}{\text{dx}^2} = \frac{1}{c^2} \frac{\text{d}^2 u}{\text{dt}^2} \).
Step by step solution
01
Understanding the given function
The function given is a combination of two functions, where: \( u = f(x - ct) + g(x + ct) \). This represents the solution as two wave functions traveling in opposite directions.
02
First partial derivative with respect to x
Differentiate both terms of the function with respect to x: \( \frac{\text{d}}{\text{dx}}[f(x - ct)] = f'(x - ct) \), \( \frac{\text{d}}{\text{dx}}[g(x + ct)] = g'(x + ct) \). So, \( \frac{\text{d}u}{\text{dx}} = \frac{\text{d}}{\text{dx}}[f(x - ct) + g(x + ct)] = f'(x - ct) + g'(x + ct) \).
03
Second partial derivative with respect to x
Differentiate the first derivative with respect to x again: \( \frac{\text{d}^2 u}{\text{dx}^2} = \frac{\text{d}}{\text{dx}}[f'(x - ct) + g'(x + ct)] = f''(x - ct) + g''(x + ct) \).
04
First partial derivative with respect to t
Differentiate the given function with respect to t: \( \frac{\text{d}}{\text{dt}}[f(x - ct)] = -c f'(x - ct) \), \( \frac{\text{d}}{\text{dt}}[g(x + ct)] = c g'(x + ct) \). So, \( \frac{\text{d}u}{\text{dt}} = \frac{\text{d}}{\text{dt}}[f(x - ct) + g(x + ct)] = -c f'(x - ct) + c g'(x + ct) \).
05
Second partial derivative with respect to t
Differentiate the first derivative with respect to t again: \( \frac{\text{d}^2 u}{\text{dt}^2} = \frac{\text{d}}{\text{dt}}[-c f'(x - ct) + c g'(x + ct)] = c^2 f''(x - ct) + c^2 g''(x + ct) \).
06
Relate the second derivatives of x and t
Compare the second derivatives obtained: \( \frac{\text{d}^2 u}{\text{dx}^2} = f''(x - ct) + g''(x + ct) \), \( \frac{\text{d}^2 u}{\text{dt}^2} = c^2 [f''(x - ct) + g''(x + ct)] \). So, \( \frac{\text{d}^2 u}{\text{dx}^2} = \frac{1}{c^2} \frac{\text{d}^2 u}{\text{dt}^2} \).
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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 tool in calculus, especially when dealing with functions of multiple variables. Unlike ordinary derivatives, which are taken with respect to a single variable in a single-variable function, partial derivatives are taken with respect to one variable while keeping other variables constant. This is particularly useful in the context of wave equations, where a function might depend on both space and time.
For example, consider the function given in the exercise: \(u = f(x - ct) + g(x + ct)\). When we take the partial derivative of \(u\) with respect to \(x\), we treat \(t\) as a constant, and vice versa.
For example, consider the function given in the exercise: \(u = f(x - ct) + g(x + ct)\). When we take the partial derivative of \(u\) with respect to \(x\), we treat \(t\) as a constant, and vice versa.
- The first partial derivative with respect to \(x\) is \( \frac{\text{d}u}{\text{dx}} = f'(x - ct) + g'(x + ct) \).
- The first partial derivative with respect to \(t\) is \( \frac{\text{d}u}{\text{dt}} = -c f'(x - ct) + c g'(x + ct) \).
Second-Order Differential Equations
Second-order differential equations involve second derivatives and are common in physics and engineering, especially when describing wave phenomena. In the given exercise, you're dealing with a linear homogeneous second-order differential equation.
The general form of the wave equation involves both spatial and temporal variables, and it requires second partial derivatives:
The general form of the wave equation involves both spatial and temporal variables, and it requires second partial derivatives:
- The second partial derivative with respect to \(x\) is \( \frac{\text{d}^2 u}{\text{dx}^2} = f''(x - ct) + g''(x + ct) \).
- The second partial derivative with respect to \(t\) is \( \frac{\text{d}^2 u}{\text{dt}^2} = c^2 f''(x - ct) + c^2 g''(x + ct) \).
Wave Functions
Wave functions are used to describe waves and oscillations in various physical contexts, from sound waves to light waves to quantum mechanical probability waves. The exercise deals with a particular form of solution to the wave equation, given by the superposition of two wave functions: \(u = f(x - ct) + g(x + ct) \).
These functions represent waves traveling in opposite directions.
These functions represent waves traveling in opposite directions.
- \