Problem 34
Question
Give an example of: A differential equation that has a trigonometric function as a solution.
Step-by-Step Solution
Verified Answer
\( \frac{d^2y}{dx^2} + y = 0 \) has the solution \( y = A\sin(x) + B\cos(x) \).
1Step 1: Understanding Differential Equations
A differential equation relates a function with its derivatives. Our task is to identify an equation where the solution involves trigonometric functions, like sine or cosine.
2Step 2: Choose a Basic Trigonometric Equation
Consider starting with the simplest trigonometric functions. The derivatives of sine and cosine functions yield each other, making them good candidates for differential equations with trigonometric solutions.
3Step 3: Identify a Specific Differential Equation
One basic differential equation with a trigonometric solution is the second-order equation: \( \frac{d^2y}{dx^2} + y = 0 \).
4Step 4: Verify the Trigonometric Solution
The general solution to \( \frac{d^2y}{dx^2} + y = 0 \) is \( y = A\sin(x) + B\cos(x) \), where \( A \) and \( B \) are constants. This shows our function involves trigonometric forms.
5Step 5: Analyze the Solution
We have shown that \( y = A\sin(x) + B\cos(x) \) satisfies the differential equation, confirming it is a suitable example where the solution involves trigonometric functions.
Key Concepts
Trigonometric FunctionsSecond-Order Differential EquationsSine and Cosine Solutions
Trigonometric Functions
Trigonometric functions are a fundamental category of functions in mathematics, often dealing with the angles and lengths of triangles. The primary trigonometric functions include sine (\( \sin \theta \) ) and cosine (\( \cos \theta \) ). They help us describe periodic phenomena such as sound waves, light waves, and the oscillations of springs. These functions repeat at regular intervals and are characterized by their unique properties:
- Periodicity: Sine and cosine functions have a period of \( 2\pi \), meaning they repeat every \( 2\pi \) units.
- Amplitudes: Their values oscillate between -1 and 1.
- Derivatives: The derivative of the sine function is the cosine, and the derivative of the cosine function is the negative sine, \( \frac{d}{dx} \sin x = \cos x \) and \( \frac{d}{dx} \cos x = -\sin x \).
Second-Order Differential Equations
Second-order differential equations are equations involving the second derivative of a function. These equations often model systems where the rate of change of a variable is itself changing, such as physical systems experiencing acceleration. The general form of a second-order differential equation is \( y'' + p(x)y' + q(x)y = g(x) \), where \( y'' \) is the second derivative of \( y \).
In particular, the equation \( \frac{d^2y}{dx^2} + y = 0 \) is a simple yet powerful second-order differential equation. It is homogeneous, meaning the right-hand side equals zero. The lack of a first derivative term simplifies the equation.
This specific equation describes many physical phenomena, such as simple harmonic motion, where the acceleration of a particle is proportional and opposite to its displacement. It highlights the self-regulating nature of harmonic oscillators, like springs or pendulums.
In particular, the equation \( \frac{d^2y}{dx^2} + y = 0 \) is a simple yet powerful second-order differential equation. It is homogeneous, meaning the right-hand side equals zero. The lack of a first derivative term simplifies the equation.
This specific equation describes many physical phenomena, such as simple harmonic motion, where the acceleration of a particle is proportional and opposite to its displacement. It highlights the self-regulating nature of harmonic oscillators, like springs or pendulums.
Sine and Cosine Solutions
When we solve the differential equation \( \frac{d^2y}{dx^2} + y = 0 \), we discover that the solutions are combinations of sine and cosine functions. The general solution is expressed as\[ y = A\sin(x) + B\cos(x) \]where \( A \) and \( B \) are constants determined by initial conditions. These constants allow the equation to adapt to different starting points and scenarios.
- Sine and cosine pairs: This pair of solutions reflects the symmetry and periodicity inherent in the equation. Each function complements the other in its contribution to the equation's overall solution.
- Initial conditions: By applying specific values at an initial point, we can solve for the constants \( A \) and \( B \), tailoring the solution to fit particular physical situations.
- Physical interpretation: For example, if describing the motion of a mass attached to a spring, these functions represent the oscillatory motion observed over time.
Other exercises in this chapter
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