Chapter 8: Problem 20
By using Laplace transforms, solve the following differential equations subject to the given initial conditions. $$y^{\prime \prime}-8 y^{\prime}+16 y=32 t, \quad y_{0}=1, y_{0}^{\prime}=2$$
Short Answer
Expert verified
The solution is \( y(t) = \frac{t^2}{2} e^{4t} + 9t e^{4t} - 4e^{4t} + 8t \).
Step by step solution
01
- Take the Laplace transform of both sides
First, take the Laplace transform of the differential equation. Recall that the Laplace transform of a derivative is: \[ \mathcal{L}\{ y' \}(s) = sY(s) - y_0 \] \[ \mathcal{L}\{ y'' \}(s) = s^2 Y(s) - s y_0 - y_0' \] Using these, the transform of the given equation is: \[ \mathcal{L}\{ y'' - 8y' + 16y \} = \mathcal{L}\{ 32t \} \] Substituting the transforms, we get: \[ (s^2 Y(s) - s y_0 - y_0') - 8 (s Y(s) - y_0) + 16 Y(s) = \frac{32}{s^2} \]
02
- Substitute initial conditions
Now substitute the given initial conditions, \( y_0 = 1 \) and \( y_0' = 2 \), into the equation: \[ (s^2 Y(s) - s \cdot 1 - 2) - 8 (s Y(s) - 1) + 16 Y(s) = \frac{32}{s^2} \] This simplifies to: \[ s^2 Y(s) - s - 2 - 8s Y(s) + 8 + 16 Y(s) = \frac{32}{s^2} \]
03
- Solve for \( Y(s) \)
Combine like terms to solve for \( Y(s) \): \[ s^2 Y(s) - 8s Y(s) + 16 Y(s) = s + 6 + \frac{32}{s^2} \] Factor out \( Y(s) \): \[ (s^2 - 8s + 16) Y(s) = s + 6 + \frac{32}{s^2} \] \[ (s - 4)^2 Y(s) = s + 6 + \frac{32}{s^2} \] Therefore, \[ Y(s) = \frac{s + 6 + \frac{32}{s^2}}{(s - 4)^2} \]
04
- Simplify the equation
Separate the terms for easier inverse Laplace transform: \[ Y(s) = \frac{s + 6}{(s - 4)^2} + \frac{32}{s^2 (s - 4)^2} \]
05
- Perform partial fraction decomposition
Finding coefficients and solving yields: \[ \frac{32}{s^2 (s - 4)^2} = \frac{8}{s^2} - \frac{4}{s} + \frac{8}{(s - 4)^2} \]
06
- Take the inverse Laplace transform
Using the inverse Laplace transform, translate each term back to the time domain: \[ y(t) = \mathcal{L}^{-1}\left\{ \frac{s + 6}{(s - 4)^2} \right\} + \mathcal{L}^{-1}\left\{ \frac{8}{s^2} \right\} - \mathcal{L}^{-1}\left\{ \frac{4}{s} \right\} + \mathcal{L}^{-1}\left\{ \frac{8}{(s - 4)^2} \right\} \] Apply the inverse transforms: \[ y(t) = \left(t + \frac{t^2}{2}\right) e^{4t} + 8t - 4e^{4t} + 8t e^{4t} \]
07
- Simplify the result
Combine like terms for the final solution: \[ y(t) = \left(t + \frac{t^2}{2} + 8t \right) e^{4t} - 4e^{4t} + 8t \] Transform it to: \[ y(t) = \frac{t^2}{2} e^{4t} + 9t e^{4t} - 4e^{4t} + 8t \] Hence the final solution is: \[ y(t) = \frac{t^2}{2} e^{4t} + 9t e^{4t} - 4e^{4t} + 8t \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Differential Equations
Differential equations involve functions and their derivatives. These equations showcase how a function changes with respect to an independent variable, typically time. For example, in physics, they describe how velocity changes over time, given acceleration. Differential equations are categorized based on their order (first, second, etc.) and linearity. The given exercise deals with a second-order linear differential equation: \(y'' - 8y' + 16y = 32t\). Here, we have the second derivative \(y''\), the first derivative \(y'\), and the function itself \(y\). Solving differential equations is crucial for modeling phenomena across various fields like engineering, physics, and economics.
Initial Conditions
Initial conditions specify the values of the function and its derivatives at the start. These are essential in finding unique solutions. In our exercise, the initial conditions are \(y(0) = 1\) and \(y'(0) = 2\). They help in simplifying the transformed differential equation. When we take the Laplace transform of the second-order differential equation, we use these initial conditions for solving the resulting algebraic equation. Initial conditions often depict starting points, such as initial temperature, population, or velocity, making the solution uniquely determined.
Inverse Laplace Transform
The Inverse Laplace Transform is used to revert back from the frequency domain to the time domain. The process involves rules and tables for common transforms. In our exercise, after solving the algebraic equation for \(Y(s)\) in the Laplace domain, we need the inverse Laplace transform to find \(y(t)\). For instance, \(\mathcal{L}^{-1} \left\{ \frac{8}{s^2} \right\} = 8t\) and \(\mathcal{L}^{-1} \left\{ \frac{8}{(s - 4)^2} \right\} = 8te^{4t}\). Understanding these inverses is crucial since it brings the physical interpretation back from the mathematical abstraction.