Chapter 6: Problem 16
Find the general solution of each differential equation or state that the differential equation is not separable. If the exercise says "and check," verify that your answer is a solution. \(y^{\prime}=e^{x}+y\)
Short Answer
Expert verified
The general solution is \( y = e^{x}(x + C) \).
Step by step solution
01
Identify the Form
The given differential equation is \( y' = e^x + y \). It is a first-order linear differential equation because it can be rewritten in the standard form \( y' - y = e^x \), where the term \( y' - y \) is linear.
02
Find the Integrating Factor
For first-order linear differential equations of the form \( y' + P(x) y = Q(x) \), the integrating factor \( \, \mu(x) = e^{\int P(x) \mathop{d}x} \, \) is used. Here, \( P(x) = -1 \), so the integrating factor is: \[\mu(x) = e^{- \int 1 \mathop{d}x} = e^{-x}.\]
03
Multiply by the Integrating Factor
Multiply both sides of the equation \( y' - y = e^x \) by the integrating factor \( e^{-x} \):\[ e^{-x} y' - e^{-x} y = e^{x} e^{-x}.\]This simplifies to: \[e^{-x} y' - e^{-x} y = 1.\]
04
Solve the Left Side as a Derivative
Recognize that \( e^{-x} y' - e^{-x} y = 1 \) can be written as a derivative:\[\frac{d}{dx}(e^{-x} y) = 1.\]
05
Integrate Both Sides
Integrate both sides with respect to \( x \):\[\int \frac{d}{dx}(e^{-x} y) \, dx = \int 1 \, dx.\]This gives:\[e^{-x} y = x + C,\]where \( C \) is an integration constant.
06
Solve for y
To find \( y \), multiply both sides by \( e^{x} \):\[y = e^{x}(x + C).\]This is the general solution of the differential equation.
07
Verify the Solution
To verify, differentiate \( y = e^{x}(x + C) \) and show it satisfies the original equation. Differentiate:\[y' = e^x(x + C) + e^x.\]Plug into the original equation:\[e^x(x + C) + e^x = e^x + e^x(x + C).\]Both sides match, confirming the solution.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Integrating Factor
When solving first-order linear differential equations, the concept of an integrating factor is crucial. This method transforms the equation into a form that is much easier to handle. Given a differential equation in the form \( y' + P(x) y = Q(x) \), we find the integrating factor, \( \mu(x) \). This factor is given by \( \mu(x) = e^{\int P(x) \, dx} \), where \( P(x) \) is a function of \( x \) derived from the equation.
For the differential equation \( y' - y = e^x \), we identify \( P(x) = -1 \). Subsequently, the integrating factor becomes \( \mu(x) = e^{\int -1 \, dx} = e^{-x} \).
By multiplying every term of the differential equation by \( e^{-x} \), we can simplify and effectively combine terms involving \( y \). This multiplication step transforms the left-hand side into the derivative of \( e^{-x} y \), enabling easier integration on both sides.
For the differential equation \( y' - y = e^x \), we identify \( P(x) = -1 \). Subsequently, the integrating factor becomes \( \mu(x) = e^{\int -1 \, dx} = e^{-x} \).
By multiplying every term of the differential equation by \( e^{-x} \), we can simplify and effectively combine terms involving \( y \). This multiplication step transforms the left-hand side into the derivative of \( e^{-x} y \), enabling easier integration on both sides.
General Solution
The general solution of a differential equation provides a family of possible solutions, capturing all specific instances with a constant that can be determined if further conditions are provided. After obtaining the integrating factor for the differential equation \( y' - y = e^x \), the equation evolves to \( e^{-x} y' - e^{-x} y = 1 \).
With this simplification in place, recognize that the left-hand side is the derivative of a product: \( \frac{d}{dx}(e^{-x} y) = 1 \).
When both sides are integrated, the result is \( e^{-x} y = x + C \), where \( C \) is an integration constant and denotes any real number. Isolate \( y \) by multiplying through by \( e^{x} \), and we derive the general solution: \( y = e^{x}(x + C) \).
This expression outlines an infinite set of solutions depending on the value of \( C \). Specific solutions can be determined if initial or boundary conditions are given.
With this simplification in place, recognize that the left-hand side is the derivative of a product: \( \frac{d}{dx}(e^{-x} y) = 1 \).
When both sides are integrated, the result is \( e^{-x} y = x + C \), where \( C \) is an integration constant and denotes any real number. Isolate \( y \) by multiplying through by \( e^{x} \), and we derive the general solution: \( y = e^{x}(x + C) \).
This expression outlines an infinite set of solutions depending on the value of \( C \). Specific solutions can be determined if initial or boundary conditions are given.
Verification of Solution
Verification is a key step to ensure that the derived solution actually satisfies the original differential equation. For our solution \( y = e^{x}(x + C) \), determining its derivative \( y' \) is necessary. Compute \( y' \) as follows: differentiate \( y = e^{x}(x + C) \) to obtain \( y' = e^x(x + C) + e^x \).
Plug \( y \) and \( y' \) back into the original equation \( y' = e^x + y \). Upon substitution, the equality \( e^x(x + C) + e^x = e^x + e^x(x + C) \) holds true. Both sides are identical, confirming that the solution satisfies the differential equation.
Through this process, verification ensures that the solution is neither a computational artifact nor an algebraic coincidence, but rather a true solution to the problem. This verification technique is a standard practice anytime solutions are claimed for differential equations, ensuring reliability of the results presented.
Plug \( y \) and \( y' \) back into the original equation \( y' = e^x + y \). Upon substitution, the equality \( e^x(x + C) + e^x = e^x + e^x(x + C) \) holds true. Both sides are identical, confirming that the solution satisfies the differential equation.
Through this process, verification ensures that the solution is neither a computational artifact nor an algebraic coincidence, but rather a true solution to the problem. This verification technique is a standard practice anytime solutions are claimed for differential equations, ensuring reliability of the results presented.