Chapter 12: Problem 3
Solve the following differential equations by power series and also by an elementary method. Verify that the series solution is the power series expansion of your other solution. $$ x y^{\prime}=x y+y $$
Short Answer
Expert verified
y = C_1 x e^x (series) matches with y = C_1 x e^x (exponential).
Step by step solution
01
Rewrite the Differential Equation
Rewrite the given differential equation in standard form. The given equation is: \[ x y^{\text{'}} = x y + y \]Divide both sides by x to get: \[ y^{\text{'}} = y + \frac{y}{x} \]
02
Separate Variables
Rewrite the equation to separate variables, putting all terms involving y on one side and all terms involving x on the other. \[ y^{\text{'}} = y + \frac{y}{x} = \left(1 + \frac{1}{x}\right) y \]Thus, \[ \frac{dy}{y} = \left(1 + \frac{1}{x}\right) dx \]
03
Integrate Both Sides
Integrate both sides of the separated equation.\[ \int \frac{1}{y} dy = \int \left(1 + \frac{1}{x}\right) dx \]This gives:\[ \ln|y| = x + \ln|x| + C \]
04
Solve for y
Exponentiate both sides to solve for y.\[ e^{\ln|y|} = e^{x + \ln|x| + C} \]This simplifies to:\[ y = e^{x} |x| e^{C} \]Letting \(e^C = C_1\), the solution is:\[ y(x) = C_1 x e^{x} \]
05
Power Series Solution Form
Assume a power series solution of the form\[ y = \sum_{n=0}^{\infty} a_n x^n \]Then, the derivative is\[ y^{\text{'}} = \sum_{n=1}^{\infty} n a_n x^{n-1} \]
06
Substitute Series into Differential Equation
Substituting these into the differential equation, we get:\[ x \sum_{n=1}^{\infty} n a_n x^{n-1} = x \sum_{n=0}^{\infty} a_n x^n + \sum_{n=0}^{\infty} a_n x^n \]Simplify and combine terms:\[ \sum_{n=1}^{\infty} n a_n x^n = \sum_{n=0}^{\infty} a_n x^{n+1} + \sum_{n=0}^{\infty} a_n x^n \]
07
Align Indexes and Compare Coefficients
Align indexes and compare coefficients of like powers of x. Set the coefficients of each power of x to zero:For \(x^0\): \[ a_0 = 0 \]For \( x^{n+1}\): \[ (n+1) a_{n+1} = a_n \]Therefore, \[ a_{n+1} = \frac{a_n}{n+1} \]and due to recursive nature, general term:\[ a_n = \frac{a_1}{n!} \]
08
Form Solution
Given the general term, the power series is:\[ y = \sum_{n=1}^{\infty} \frac{a_1}{n!} x^n = a_1 \sum_{n=1}^{\infty} \frac{x^n}{n!} \]This simplifies using known series for the exponential function:\[ y = a_1 (e^x - 1) \]Since an arbitrary constant can be redefined, let \(a_1 = C_1\).\[ y = C_1 (e^x - 1) \]
09
Verify Power Series with Exponential Solution
Verify that the obtained power series solution matches the original solution.Original exponential solution:\[ y = C_1 x e^x \]Power series solution:\[ y = C_1 x e^x \]Both methods give a consistent solution.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
power series
To understand how power series are used in solving differential equations, we begin with the concept itself. A power series is an infinite series of the form: \[ y = \sum_{n=0}^{\infty} a_n x^n \] where \( a_n \) are coefficients and \( x^n \) are powers of \( x \).
This allows us to express a function as an infinite sum of terms in powers of \( x \).
In the context of solving differential equations, we assume that the solution can be expressed as a power series.
We then find the coefficients \( a_n \) step by step, using given initial conditions and other constraints..
For example, if you start with \( y = \sum_{n=0}^{\infty} a_n x^n \), its derivative is \( y' = \sum_{n=1}^{\infty} n a_n x^{n-1} \).
Substituting these into the differential equation, we align indexes, compare coefficients, and solve for the coefficients \( a_n \).
This approach helps in finding a series representation for the solution.
This allows us to express a function as an infinite sum of terms in powers of \( x \).
In the context of solving differential equations, we assume that the solution can be expressed as a power series.
We then find the coefficients \( a_n \) step by step, using given initial conditions and other constraints..
For example, if you start with \( y = \sum_{n=0}^{\infty} a_n x^n \), its derivative is \( y' = \sum_{n=1}^{\infty} n a_n x^{n-1} \).
Substituting these into the differential equation, we align indexes, compare coefficients, and solve for the coefficients \( a_n \).
This approach helps in finding a series representation for the solution.
separation of variables
Separation of variables is a key technique to solve differential equations.
The idea is to rewrite the equation in such a way that all terms involving one variable appear on one side of the equation, and all terms involving the other variable appear on the other side.
Consider the given equation: \[ x y^{\'} = x y + y \] By dividing both sides by \( x \), we get: \( y^{\'} = y + \frac{y}{x} \).Next, rewriting this to separate variables, we have \( \frac{dy}{y} = (1 + \frac{1}{x})dx \).
Once the variables are separated, we integrate both sides to find the solution.
This process involves two main steps: separating the variables and then integrating both sides.
By integrating both sides, we often end up with a natural logarithm or an exponential expression, which we can solve further to find the function \( y \).
The idea is to rewrite the equation in such a way that all terms involving one variable appear on one side of the equation, and all terms involving the other variable appear on the other side.
Consider the given equation: \[ x y^{\'} = x y + y \] By dividing both sides by \( x \), we get: \( y^{\'} = y + \frac{y}{x} \).Next, rewriting this to separate variables, we have \( \frac{dy}{y} = (1 + \frac{1}{x})dx \).
Once the variables are separated, we integrate both sides to find the solution.
This process involves two main steps: separating the variables and then integrating both sides.
By integrating both sides, we often end up with a natural logarithm or an exponential expression, which we can solve further to find the function \( y \).
exponential function
The exponential function \( e^x \) plays a crucial role in solving differential equations.
It's a key function, often arising when solving equations involving growth or decay processes.
In our differential equation solution, after integrating both sides, we obtained \ln|y| = x + \ln|x| + C.\This simplification involves exponentiating both sides:
\[ e^{\ln|y|} = e^{x + \ln|x| + C} \]
The laws of exponents allow us to write this as:
\( y = e^x |x| e^C \)
Letting \( e^C = C_1 \), the solution simplifies to \( y = C_1 x e^x \).
The exponential function thus provides a way to simplify and solve the differential equation, leading us to the final solution.
It's a key function, often arising when solving equations involving growth or decay processes.
In our differential equation solution, after integrating both sides, we obtained \ln|y| = x + \ln|x| + C.\This simplification involves exponentiating both sides:
\[ e^{\ln|y|} = e^{x + \ln|x| + C} \]
The laws of exponents allow us to write this as:
\( y = e^x |x| e^C \)
Letting \( e^C = C_1 \), the solution simplifies to \( y = C_1 x e^x \).
The exponential function thus provides a way to simplify and solve the differential equation, leading us to the final solution.
integration
Integration is the process of finding the integral of a function.
It's used extensively to solve differential equations.
In our exercise, we separated the variables to integrate both sides of the equation:
\( \int \frac{1}{y} dy = \int (1 + \frac{1}{x}) dx \)
This step-by-step integration allows us to find \ln|y| = x + \ln|x| + C.\Once we perform the integration, we solve for the arbitrary constant \( C \) using initial conditions.
This leads us closer to the final solution of the differential equation.
In this exercise, after integrating both sides, we determined that \( y = C_1 x e^x \).
Integrating properly helps us transition from a differential equation to finding a function that satisfies the given conditions.
It's used extensively to solve differential equations.
In our exercise, we separated the variables to integrate both sides of the equation:
\( \int \frac{1}{y} dy = \int (1 + \frac{1}{x}) dx \)
This step-by-step integration allows us to find \ln|y| = x + \ln|x| + C.\Once we perform the integration, we solve for the arbitrary constant \( C \) using initial conditions.
This leads us closer to the final solution of the differential equation.
In this exercise, after integrating both sides, we determined that \( y = C_1 x e^x \).
Integrating properly helps us transition from a differential equation to finding a function that satisfies the given conditions.