/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 15 Find the general solution. $$y... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Find the general solution. $$y^{\prime}-e^{x} y=0$$

Short Answer

Expert verified
The general solution to the given differential equation \(y' - e^x y = 0\) is \(y(x) = Ce^{e^x}\), where C is the integration constant.

Step by step solution

01

Put the differential equation in standard form

We are given the differential equation: \(y' - e^x y = 0\). We need to rewrite this equation in the standard form for first-order linear differential equations: \[y' + P(x) y = Q(x)\] Here, we can see that: \(P(x) = -e^x\) and \(Q(x) = 0\).
02

Compute the integrating factor

The integrating factor, denoted by µ(x), is given by the formula: \[\mu(x) = e^{\int P(x) dx}\] So in our case, we need to find the integrating factor by calculating the integral of P(x) = \(-e^x\): \[\mu(x) = e^{\int - e^x dx}\] To integrate \(- e^x\), we will get: \[\int - e^x dx = -e^x + C\] Now we can substitute back into our equation for the integrating factor: \[\mu(x) = e^{-e^x + C}\] The constant term C can be absorbed inside the integrating factor (because we're only interested in the equation's format), so we can write: \[\mu(x) = e^{-e^x}\]
03

Multiply the equation by the integrating factor

Now, we need to multiply both sides of our standard form equation by the integrating factor \(\mu(x) = e^{-e^x}\): \[e^{-e^x}(y' - e^x y) = 0\] After multiplying, we get: \[e^{-e^x} y' - y = 0\]
04

Integrate both sides of the equation

Now, let's integrate both sides of the equation: \[\int (e^{-e^x} y' - y) dx = \int 0 dx\] Here, we can recognize that the left side is actually the derivative of the product of y(x) and the integrating factor (recall the product rule for derivatives): \[\frac{d}{dx}(y(x)e^{-e^x}) = e^{-e^x} y' - y\] So we can rewrite our integral as: \[\frac{d}{dx}(y(x)e^{-e^x}) = 0\] Now, we integrate both sides: \[\int\frac{d}{dx}(y(x)e^{-e^x})dx = \int 0 dx\] This yields: \[y(x)e^{-e^x} = C\] where C is the integration constant.
05

Solve for y(x)

Finally, we can solve for y(x) by dividing both sides by \(e^{-e^x}\): \[y(x) = Ce^{e^x}\] This is the general solution to the given differential equation.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Integrating Factor
When dealing with first-order linear differential equations, just like the one given in the problem \(y' - e^x y = 0\), it is often helpful to transform it into an easier format for solving.The standard form looks like this: \(y' + P(x) y = Q(x)\).In this format, \(P(x) = -e^x\) and \(Q(x) = 0\).The integrating factor is a powerful tool to simplify such equations.To find the integrating factor, we use the formula \(\mu(x) = e^{\int P(x) \, dx}\).It is a multiplier that we apply to the entire differential equation.By doing so, it allows us to express the left side of the equation as the derivative of a product.In our example, we calculated:
  • \(\int - e^x \, dx = - e^x + C\)
  • \(\mu(x) = e^{-e^x}\)
Using this integrating factor, we simplify the original equation, making it ready for further operations.
General Solution
Finding the general solution of a differential equation involves solving it in a way that includes all possible solutions.In our exercise, once transformed using the integrating factor, the differential equation becomes simpler to solve.After multiplying \(y' - e^x y = 0\) by \(e^{-e^x}\), we get:\(e^{-e^x} y' - y = 0\).Recognizing this as a derivative of a product, we rewrite:\(\frac{d}{dx}(y(x)e^{-e^x}) = 0\).Integrating both sides, we obtain:\(y(x)e^{-e^x} = C\),where \(C\) is a constant of integration.This integration captures every possible solution by including this arbitrary constant.Finally, isolating \(y(x)\), we find:\(y(x) = Ce^{e^x}\).This is the general solution of the differential equation, encompassing all potential shifts via \(C\).
Product Rule for Derivatives
The product rule for derivatives is an essential concept, particularly when solving differential equations like the one provided.This rule states that if you have two functions, \(u(x)\) and \(v(x)\), the derivative of their product is:\((uv)' = u'v + uv'\).In the context of our problem:
  • The product is \(y(x)e^{-e^x}\).
  • The derivative became the expression \(e^{-e^x} y' - y\).
The beauty here is that we adjusted the equation into a perfect derivative using the integrating factor, which disguises a part of the expression as a product derivative.By recognizing the structure of \(e^{-e^x} y' - y\) as a derivative,we connected it back to its integral form: \(\frac{d}{dx}(y(x)e^{-e^x}) = 0\).Understanding this principle further facilitates integrating separately and simplifying to reach the general solution.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Show that the general solution of the differential equation $$y^{\prime \prime}+\omega^{2} y=0$$ can be written $$y=A \sin \left(\omega x+\phi_{0}\right)$$

A 200 -liter tank, initially full of water, develops u leak at the bottom. Given that \(20 \%\) of the water leaks out in the first 5 minutes, find the amount of water left in the tank \(t\) minutes after the leak develops: (a) if the water drains off at a rate proportional to the amount of water present. (b) if the water drains off at a rate proportional to the product of the time elapsed and the amount of water present.

Suppose that the roots \(r_{1}\) and \(r_{2}\) of the characteristic equation are real and instinct. Then they can be written as \(r_{1}=\alpha+\beta\) and \(r_{2}=\alpha-\beta,\) where \(\alpha\) and \(\beta\) are real. Show that the general solution of the homogeneous equation can be expressed in the form $$y=e^{x x}\left(C_{1} \cosh \beta x+C_{2} \sinh \beta x\right)$$

An object falling from rest in air is subject not only to gravitational force but also to air resistance. Assume that the air resistance is proportional to the velocity and acts in a direction opposite to the motion. Then the velocity of the object at time \(t\) satisfies an equation of the form $$ v^{\prime}=32-k \nu $$ where \(k\) is a positive constant and \(v(0)-0 .\) Here we are measuring distance in feet and the positive direction is down. (a) Find \(v(t)\) (b) Show that \(v(t)\) cannot exceed \(32 / k\) and that \(v(t) \rightarrow\) $$ 32 / k \text { as } t \rightarrow \infty $$ (c) Sketch the graph of \(v\)

Solve the initial-value problem. $$\frac{d y}{d x}=x \sqrt{\frac{1-y^{2}}{1-x^{2}}}, \quad y(0)=0.$$

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.