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Find the general solution to the differential equation. $$y^{\prime \prime}-4 y=4 e^{2 t}$$

Short Answer

Expert verified
The general solution is \( y = C_1e^{2t} + C_2e^{-2t} + 2te^{2t} \).

Step by step solution

01

Identify the Type of Differential Equation

The given differential equation is \( y'' - 4y = 4e^{2t} \). It is a second-order linear non-homogeneous differential equation with constant coefficients.
02

Solve the Homogeneous Equation

First, consider the homogeneous equation \( y'' - 4y = 0 \). To solve it, assume a trial solution of the form \( y_h = e^{rt} \), which gives the characteristic equation \( r^2 - 4 = 0 \). Solving this, we find \( r = \pm 2 \). Therefore, the general solution for the homogeneous equation is \( y_h = C_1e^{2t} + C_2e^{-2t} \).
03

Find a Particular Solution to the Non-Homogeneous Equation

To find a particular solution, \( y_p \), assume a form based on the non-homogeneous part \( 4e^{2t} \). Try \( y_p = Ate^{2t} \) as the particular solution. Compute \( y_p' = Ae^{2t} + 2Ate^{2t} \) and \( y_p'' = 2Ae^{2t} + 4Ate^{2t} \). Substitute into the original differential equation \( y_p'' - 4y_p = 4e^{2t} \) to find \( A \). This results in \( 2Ae^{2t} = 4e^{2t} \), so \( A = 2 \). Thus, \( y_p = 2te^{2t} \).
04

Write the General Solution

Combine the homogeneous and particular solutions to form the general solution: \( y = y_h + y_p = C_1e^{2t} + C_2e^{-2t} + 2te^{2t} \), where \( C_1 \) and \( C_2 \) are arbitrary constants.

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Key Concepts

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

Linear Differential Equation
A linear differential equation is characterized by its linear form; it means that each term involving the unknown function and its derivatives is linear or proportional. In simpler terms, the equation never contains terms like \(y^2\), \(y'\cdot y\), or any non-linear combination of \(y\), \(y'\), etc. For example, the equation \( y'' - 4y = 4e^{2t} \) is linear because all terms involving \(y\) and its derivatives are simply lined up in a standard fashion.

There are several key points to remember about linear differential equations:

  • They can be homogeneous or non-homogeneous depending on whether there is an additional function added to the equation as we see with \( 4e^{2t} \) in our example.
  • The solution method often involves solving both a homogeneous and a non-homogeneous part separately.
Understanding the linearity of a differential equation makes solving it systematic and predictable, involving well-defined steps like finding characteristic solutions and particular solutions.

The predictability of linear differential equations makes them a frequent subject of study in mathematical courses.
Characteristic Equation
The characteristic equation is a vital tool for solving linear differential equations, particularly those that are homogeneous. When faced with a differential equation like \( y'' - 4y = 0 \), we look for solutions of the form \( y_h = e^{rt} \), which transforms the differential equation into an algebraic equation for \( r \).

For the given homogeneous equation, we substitute \( y_h = e^{rt} \) into \( y'' - 4y = 0 \). This substitution leads us to the characteristic equation:

\[ r^2 - 4 = 0 \]

Solving this quadratic equation gives us roots, in this case, \( r = \pm 2 \). These roots lead to the solution of the homogeneous differential equation. The general solution based on these roots is a combination:

\[ y_h = C_1e^{2t} + C_2e^{-2t} \]

This is a critical step since it constructs the groundwork on which particular solutions for non-homogeneous parts are added later.

Ultimately, the characteristic equation simplifies the complexity of differential equations by breaking them down into simpler algebraic problems.
Non-Homogeneous Differential Equation
A non-homogeneous differential equation includes an additional function making it more complex than just time derivatives and direct terms linked with the function. In the problem \( y'' - 4y = 4e^{2t} \), the \( 4e^{2t} \) represents this added complexity.

To solve non-homogeneous equations, we still solve the homogeneous counterpart first, which we've already discussed. The key challenge here is to find a "particular solution" that accounts for the non-zero function.

The general approach involves assuming a form for the particular solution that closely resembles the non-homogeneous part. In this example, because \( 4e^{2t} \) is involved, a logical trial solution might be \( y_p = Ate^{2t} \). The variable \( t \) gets introduced in the trial due to exponential terms matching those we've already accounted for in the homogeneous solution; this helps avoid duplication.

Once a suitable particular solution is found, it and the homogeneous solution combine to form the full solution to the original non-homogeneous equation.
Particular Solution
Finding a particular solution is imperative when tackling non-homogeneous differential equations. It bridges the gap between the homogeneous part solved earlier and the extra function present on the equation's right side.

For our equation, \( y'' - 4y = 4e^{2t} \), we need to assume a particular solution format. Given the form \( 4e^{2t} \), a logical choice is \( y_p = Ate^{2t} \) since it mirrors the non-homogeneous term while avoiding the simple repetition of a component covered in the homogeneous solution.

To confirm our guess, take derivatives \( y_p' = Ae^{2t} + 2Ate^{2t} \) and \( y_p'' = 2Ae^{2t} + 4Ate^{2t} \), plugging them into the original equation:\
\[ y_p'' - 4y_p = 4e^{2t} \]

Matching coefficients, we find \( A = 2 \), leading to \( y_p = 2te^{2t} \).

This particular solution, tailored to the non-homogeneous function's form, when combined with the homogeneous solution, provides the comprehensive solution we seek.

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