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Solve the initial value problem. \(y^{\prime \prime}(t)+2 y^{\prime}(t)+5 y(t)=4 e^{-t}\), with \(y(0)=1\) and \(y^{\prime}(0)=1\).

Short Answer

Expert verified
The solution is \( y(t) = e^{-t}(\cos(2t) + \sin(2t) + 1) \).

Step by step solution

01

Characteristic Equation

First, solve the homogeneous part of the differential equation. Consider the equation: \( y''(t) + 2y'(t) + 5y(t) = 0 \). To find the characteristic equation, assume a solution of the form \( y_h(t) = e^{rt} \). Substituting into the homogeneous equation gives the characteristic equation \( r^2 + 2r + 5 = 0 \).
02

Solve the Characteristic Equation

Solve the quadratic \( r^2 + 2r + 5 = 0 \) using the quadratic formula \( r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \). Here \( a = 1 \), \( b = 2 \), and \( c = 5 \). This simplifies to \( r = \frac{-2 \pm \sqrt{4 - 20}}{2} \). We get \( r = -1 \pm 2i \).
03

Form the General Solution for Homogeneous Equation

Since the roots are complex, the general solution of the homogeneous equation is \( y_h(t) = e^{-t} (C_1 \cos(2t) + C_2 \sin(2t)) \), where \( C_1 \) and \( C_2 \) are constants.
04

Find Particular Solution

To find the particular solution \( y_p(t) \), guess a form based on the non-homogeneous term. Since the non-homogeneous term is \( 4e^{-t} \), try \( y_p(t) = Ae^{-t} \). Compute derivatives \( y'_p(t) = -Ae^{-t} \) and \( y''_p(t) = Ae^{-t} \). Substitute into the differential equation: \( Ae^{-t} - 2Ae^{-t} + 5Ae^{-t} = 4e^{-t} \) simplifies to \( 4Ae^{-t} = 4e^{-t} \) giving \( A = 1 \). Thus, \( y_p(t) = e^{-t} \).
05

Combine Solutions

The general solution is \( y(t) = y_h(t) + y_p(t) = e^{-t}(C_1 \cos(2t) + C_2 \sin(2t)) + e^{-t} \). Factor out \( e^{-t} \): \( y(t) = e^{-t}(C_1 \cos(2t) + C_2 \sin(2t) + 1) \).
06

Apply Initial Conditions

Use the initial conditions to find \( C_1 \) and \( C_2 \). Plugging \( y(0) = 1 \) into the general solution gives: \( 1 = 1 + C_1 \Rightarrow C_1 = 0 \). Compute the derivative \( y'(t) \), and use \( y'(0) = 1 \) to find \( C_2 \). Differentiating and setting \( t = 0 \) gives \( y'(0) = -1 * 1 + 2C_2 \) resulting in \( 1 = -1 + 2C_2 \Rightarrow C_2 = 1 \).
07

Final Solution

Substitute \( C_1 = 0 \) and \( C_2 = 1 \) into the general solution: \( y(t) = e^{-t}(\cos(2t) + \sin(2t) + 1) \). This is the solution to the initial value problem.

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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 (IVP) is a type of differential equation that comes with specific conditions called initial conditions.
These conditions allow us to find a unique solution to the differential equation.
In this exercise, the differential equation is given along with the initial conditions, which are values for the function and its derivative at a specific point. For the problem at hand, we're dealing with:
  • The differential equation: \[y''(t) + 2y'(t) + 5y(t) = 4 e^{-t}\]
  • The initial conditions: \(y(0) = 1\) and \(y'(0) = 1\)
These initial conditions are essential because they help in determining the specific constants in our general solution, thereby narrowing it down to a particular solution that fits the given problem. Without these conditions, we can only derive a general solution that could fit an unlimited number of situations.
Homogeneous Equation
A Homogeneous Equation is a natural part of solving linear differential equations.
In this context, a homogeneous equation means a differential equation set equal to zero.The homogeneous part of the given problem is: \[y''(t) + 2y'(t) + 5y(t) = 0\] This part is separated from the non-homogeneous part (the part involving \(4 e^{-t}\)).
By tackling this homogeneous equation separately, we can find the complementary or general solution. Its roots can help solve the entire differential equation.For our specific case, dealing with complex roots:
  • If roots are real and distinct: Solutions often involve exponential functions with constant coefficients.
  • If roots are complex: Solutions involve a combination of sine and cosine functions with exponential parts.
Particular Solution
Finding the Particular Solution is crucial for solving non-homogeneous differential equations.
The particular solution is needed to address the non-zero side of the equation.In our exercise, the non-homogeneous term is \(4 e^{-t}\), suggesting that the function itself is part of our guess for the particular solution:
  • We start by assuming: \(y_p(t) = Ae^{-t}\)
  • Compute its derivatives and substitute back into the differential equation.
This straightforward process yields an equation where we can solve for \(A\), ensuring that the particular solution, \(y_p(t)\), satisfies the original equation.
In this scenario, we've found that \(A=1\), leading to the particular solution \(y_p(t) = e^{-t}\).
Characteristic Equation
The Characteristic Equation is a fundamental tool for analyzing and solving linear differential equations.
It comes into play when dealing with homogeneous equations.For our exercise, after isolating the homogeneous part:
  • Assume a solution form: \(y_h(t) = e^{rt}\)
  • Substitute back into the homogeneous equation to form a polynomial equation, known as the characteristic equation.
Given the equation: \[r^2 + 2r + 5 = 0\] We solve it to find the roots using the quadratic formula: \[r = \frac{-2 \pm \sqrt{4 - 20}}{2}\] The complex roots \(-1 \pm 2i\) indicate that our general solution will involve exponential, sine, and cosine terms: \[y_h(t) = e^{-t}(C_1 \cos(2t) + C_2 \sin(2t))\] This step sets the stage for combining with the particular solution to form the final solution.

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