Problem 49
Question
The Laplace transform \(\mathscr{L}\left\\{e^{-r^{2}}\right\\}\) exists, but without finding it solve the initial-value problem $$ y^{\prime \prime}+9 y=3 e^{-t^{2}}, y(0)=0, y^{\prime}(0)=0 $$
Step-by-Step Solution
Verified Answer
The solution is \( y(t) = 3 \int_0^t \sin(3(t-v))e^{-v^2} \, dv \).
1Step 1: Transform the Differential Equation
First, apply the Laplace transform to the given differential equation: \( y''(t) + 9y(t) = 3e^{-t^2} \). Recall that the Laplace transform of a second derivative is \( \mathscr{L}\{y''(t)\} = s^2Y(s) - sy(0) - y'(0) \). Since \( y(0) = 0 \) and \( y'(0) = 0 \), this simplifies to \( s^2Y(s) \). Therefore, we have:\[ s^2Y(s) + 9Y(s) = 3\mathscr{L}\{e^{-t^2}\} \].
2Step 2: Factor the Equation for Y(s)
Factor the terms with \( Y(s) \) in the equation obtained from the Laplace transform. This results in:\[ Y(s)(s^2 + 9) = 3\mathscr{L}\{e^{-t^2}\} \].
3Step 3: Solve for Y(s)
Solve for \( Y(s) \) by dividing both sides by \( s^2 + 9 \):\[ Y(s) = \frac{3}{s^2 + 9} \mathscr{L}\{e^{-t^2}\} \].
4Step 4: Identify the Inverse Laplace Transform
Given \( Y(s) = \frac{3}{s^2 + 9} \mathscr{L}\{e^{-t^2}\} \), we need to find the inverse Laplace transform of this expression to solve for \( y(t) \). The expression \( \frac{3}{s^2 + 9} \) represents the Laplace transform of \( \sin(3t) \). Therefore, the inverse Laplace transform of \( Y(s) \) can be expressed as:\[ y(t) = 3 \int_0^t \sin(3(t-v)) f(v) \, dv \]where \( f(t) = e^{-t^2} \).
5Step 5: Express the Integral Solution
Replace \( f(v) \) with its corresponding function \( e^{-v^2} \) in the integral to describe the solution:\[ y(t) = 3 \int_0^t \sin(3(t-v))e^{-v^2} \, dv \].
6Step 6: Interpret the Solution
This integral expression provides the solution \( y(t) \) for the given initial-value problem. Since \( \mathscr{L}\{e^{-t^2}\} \) was not explicitly calculated, the expression represents a solution in terms of convolution integrals.
Key Concepts
Initial-value problemInverse Laplace TransformDifferential Equation
Initial-value problem
An initial-value problem is a type of differential equation accompanied by specific conditions that must be met by the solution. These conditions, known as initial conditions, specify values for the function and its derivatives at a particular point.
In our specific problem, the differential equation is:
Initial-value problems are common in physics and engineering, as they model how systems evolve from given starting states. Solving them typically involves methods like separation of variables, characteristic equations, or as in this exercise, using Laplace transforms.
In our specific problem, the differential equation is:
- \(y''+9y=3e^{-t^2}\)
- \(y(0)=0\)
- \(y'(0)=0\)
Initial-value problems are common in physics and engineering, as they model how systems evolve from given starting states. Solving them typically involves methods like separation of variables, characteristic equations, or as in this exercise, using Laplace transforms.
Inverse Laplace Transform
The Inverse Laplace Transform is a crucial concept that allows us to move from the Laplace domain back to the time domain. It is essentially the reverse operation of the Laplace Transform. The goal is to retrieve the original function of time which has been transformed.
In the provided exercise, we are given the expression:
The term \(\frac{3}{s^2 + 9}\) is recognized as the Laplace transform of \(3\sin(3t)\). Applying the Inverse Laplace Transform involves calculating:
In the provided exercise, we are given the expression:
- \(Y(s) = \frac{3}{s^2 + 9} \mathscr{L}\{e^{-t^2}\}\)
The term \(\frac{3}{s^2 + 9}\) is recognized as the Laplace transform of \(3\sin(3t)\). Applying the Inverse Laplace Transform involves calculating:
- \(y(t) = 3 \int_0^t \sin(3(t-v)) e^{-v^2} \ dv\)
Differential Equation
Differential equations are equations that involve an unknown function and its derivatives. They are incredibly important in modeling a wide variety of real-world phenomena such as physical systems in engineering, population dynamics in biology, and financial markets in economics.
In our case, the differential equation:
The presence of the term \(3e^{-t^2}\) on the right-hand side makes this a non-homogeneous differential equation, as it’s not solely dependent on \(y\) or its derivatives. Solving it typically involves using techniques like the method of undetermined coefficients, variation of parameters, or Laplace transforms.
Converting the differential equation into the Laplace domain can simplify solving it, especially when initial conditions are involved, as it transforms differential equations into algebraic ones. This is why Laplace transforms are such a powerful tool in handling complex initial-value problems.
In our case, the differential equation:
- \(y'' + 9y=3e^{-t^2}\)
The presence of the term \(3e^{-t^2}\) on the right-hand side makes this a non-homogeneous differential equation, as it’s not solely dependent on \(y\) or its derivatives. Solving it typically involves using techniques like the method of undetermined coefficients, variation of parameters, or Laplace transforms.
Converting the differential equation into the Laplace domain can simplify solving it, especially when initial conditions are involved, as it transforms differential equations into algebraic ones. This is why Laplace transforms are such a powerful tool in handling complex initial-value problems.
Other exercises in this chapter
Problem 48
Find either \(F(s)\) or \(f(t)\), as indicated. $$ \mathscr{L}^{-1}\left\\{\frac{e^{-2 s}}{s^{2}(s-1)}\right\\} $$
View solution Problem 48
Suppose that \(\mathscr{L}\left\\{f_{1}(t)\right\\} \quad F_{1}(s)\) for \(s>c_{1}\) and that \(\mathscr{L}\left\\{f_{2}(t)\right\\} \quad F_{2}(s)\) for \(s>c_
View solution Problem 50
Solve the integral equation $$ f(t)=e^{t}+e^{t} \int_{0}^{t} e^{-\tau} f(\tau) d \tau $$
View solution Problem 53
The function \(f(t) \quad 2 t e^{t^{2}} \cos e^{t^{2}}\) is not of exponential order. Nevertheless, show that the Laplace transform \(\mathscr{L}\left\\{2 t e^{
View solution