Chapter 8: Problem 15
Use the Laplace transform to solve the initial value problem. \(y^{\prime \prime}+3 y^{\prime}+2 y=e^{t}, \quad y(0)=0, \quad y^{\prime}(0)=1\)
Short Answer
Expert verified
Answer: The solution to the given initial value problem is \(y(t) = -\frac{1}{3}e^{-t} + \frac{2}{3}e^{-2t} + \frac{1}{3}e^t\).
Step by step solution
01
Laplace transform of both sides of the equation
To solve the initial value problem, we first need to determine the Laplace transform of both sides of the equation. This can be done using known Laplace transform properties.
Given:
\(y''(t) + 3y'(t) + 2y(t) = e^t\)
Taking Laplace transform:
\(L[y''(t)] + 3L[y'(t)] + 2L[y(t)] = L[e^t]\)
Using Laplace Transform properties for division and known transforms:
\(Lf(s)[y''] = s^2 Y(s) - sy(0) - y'(0)\)
\(Lf(s)[y'] = s Y(s) - y(0)\)
\(Lf(s)[y] = Y(s)\)
\(Lf(s)[e^t] = \frac{1}{s-1}\)
With the given initial conditions \(y(0) = 0\) and \(y'(0) = 1\):
\(s^2 Y(s) - s(0) - 1 + 3[sY(s) - 0] + 2Y(s) = \frac{1}{s-1}\)
02
Solve the algebraic Laplace domain equation
Now, we need to solve the equation for Y(s):
\( s^2 Y(s) - 1 + 3s Y(s) + 2Y(s) = \frac{1}{s-1}\)
Combine the Y(s) terms:
\((s^2 + 3s + 2) Y(s) = 1 + \frac{1}{s-1}\)
Divide by the polynomial factor:
\(Y(s) = \frac{1 + \frac{1}{s-1}}{s^2 + 3s + 2}\)
03
Inverse Laplace transform
Now we need to find the inverse Laplace transform of Y(s) to get y(t). To do this, we first need to perform partial fraction decomposition.
\(\frac{1 + \frac{1}{s-1}}{s^2 + 3s + 2} = \frac{1}{s^2 + 3s + 2} + \frac{1}{(s-1)(s^2 + 3s + 2)}\)
\(= \frac{A}{s+1} + \frac{B}{s+2} + \frac{C}{s-1}\)
Now we will solve for A, B, and C.
By doing the partial fraction expansion, we find:
\(A = -\frac{1}{3}\)
\(B = \frac{2}{3}\)
\(C = \frac{1}{3}\)
So \(Y(s) = -\frac{1}{3}\frac{1}{s+1} + \frac{2}{3}\frac{1}{s+2} + \frac{1}{3}\frac{1}{s-1}\)
Taking the inverse Laplace transform of Y(s) to obtain y(t) :
\(y(t) = L^{-1}[Y(s)] = -\frac{1}{3}e^{-t} + \frac{2}{3}e^{-2t} + \frac{1}{3}e^t\)
04
Confirm with initial conditions
Finally, we must confirm if the solution fits in the given initial conditions:
\(y(0) = -\frac{1}{3}e^0 + \frac{2}{3}e^0 + \frac{1}{3}e^0 = 0\)
\(y'(t) = \frac{1}{3}e^t - \frac{2}{3}e^{-2t} - \frac{1}{3}e^{-t}\)
\(y'(0) = \frac{1}{3}e^0 - \frac{2}{3}e^0 - \frac{1}{3}e^0 = 1\)
Both initial conditions hold true.
The solution of the given initial value problem is:
\(y(t) = -\frac{1}{3}e^{-t} + \frac{2}{3}e^{-2t} + \frac{1}{3}e^t\)
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Initial Value Problem
An initial value problem in differential equations is a problem where we need to find a function that satisfies a differential equation and also meets specific initial conditions. This means we're not only interested in finding a general solution to a differential equation but also a particular one that starts at a specified point.
For example, in the given exercise, we need to solve the differential equation \(y'' + 3y' + 2y = e^t\) while ensuring that at \(t = 0\), \(y(0) = 0\) and \(y'(0) = 1\). These initial conditions help to pinpoint the exact trajectory of our solution out of the infinitely many that the differential equation might allow.
For example, in the given exercise, we need to solve the differential equation \(y'' + 3y' + 2y = e^t\) while ensuring that at \(t = 0\), \(y(0) = 0\) and \(y'(0) = 1\). These initial conditions help to pinpoint the exact trajectory of our solution out of the infinitely many that the differential equation might allow.
Partial Fraction Decomposition
Partial fraction decomposition is a method used in algebra to break down complex rational expressions into simpler ones. This is particularly useful when dealing with expressions that are hard to manage in their original form.
In the context of inverse Laplace transforms, we aim to split a complex function into simpler parts whose inverse transforms are already known or easier to compute.
In our exercise, the expression \(\frac{1 + \frac{1}{s-1}}{s^2 + 3s + 2}\) can be broken down into \(\frac{A}{s+1} + \frac{B}{s+2} + \frac{C}{s-1}\).
By finding the constants \(A\), \(B\), and \(C\), we simplify the problem of taking the inverse Laplace transform.
In the context of inverse Laplace transforms, we aim to split a complex function into simpler parts whose inverse transforms are already known or easier to compute.
In our exercise, the expression \(\frac{1 + \frac{1}{s-1}}{s^2 + 3s + 2}\) can be broken down into \(\frac{A}{s+1} + \frac{B}{s+2} + \frac{C}{s-1}\).
By finding the constants \(A\), \(B\), and \(C\), we simplify the problem of taking the inverse Laplace transform.
Inverse Laplace Transform
The inverse Laplace transform takes us back to the time domain from the s-domain, where the Laplace transform operates. This concept helps to find a time-domain function (i.e., \(y(t)\)) from its Laplace-transformed version.
After partial fraction decomposition, the remaining task is to find the inverse Laplace transform of each term separately.
Thanks to standard Laplace transform tables and known inverse transforms, finding \(L^{-1}\) for simple fractions like \(\frac{1}{s-a}\), which yields \(e^{at}\), becomes straightforward.
Thus, in the exercise, we find that \(-\frac{1}{3}e^{-t}\), \(\frac{2}{3}e^{-2t}\), and \(\frac{1}{3}e^{t}\) are the inverse transforms of the decomposed parts of \(Y(s)\).
After partial fraction decomposition, the remaining task is to find the inverse Laplace transform of each term separately.
Thanks to standard Laplace transform tables and known inverse transforms, finding \(L^{-1}\) for simple fractions like \(\frac{1}{s-a}\), which yields \(e^{at}\), becomes straightforward.
Thus, in the exercise, we find that \(-\frac{1}{3}e^{-t}\), \(\frac{2}{3}e^{-2t}\), and \(\frac{1}{3}e^{t}\) are the inverse transforms of the decomposed parts of \(Y(s)\).
Differential Equations
Differential equations involve functions and their derivatives, and they describe how a function changes. They are critical in modeling numerous scenarios in physics, economics, and engineering where change is a fundamental characteristic.
In our exercise, the differential equation \(y'' + 3y' + 2y = e^t\) is linear, as it involves no powers or products of the function or its derivatives.
Solving such equations typically requires techniques like the Laplace transform, which helps in transforming complex differential equations into simpler algebraic forms.
This transformation allows means to handle initial conditions straightforwardly in solving the equation by taking the inverse Laplace after simplifying via partial fraction decomposition.
In our exercise, the differential equation \(y'' + 3y' + 2y = e^t\) is linear, as it involves no powers or products of the function or its derivatives.
Solving such equations typically requires techniques like the Laplace transform, which helps in transforming complex differential equations into simpler algebraic forms.
This transformation allows means to handle initial conditions straightforwardly in solving the equation by taking the inverse Laplace after simplifying via partial fraction decomposition.