Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

. Show that if \(y=u e^{\alpha x}\) is assumed to be a solution of \(a^{2} d^{2} y+a d y d x+y d x^{2}=0\), then if \(\alpha=-1 / 2 a\), conclude that \(u\) is a solution to \(a^{2} d^{2} u+(3 / 4) u d x^{2}=0\).

Short Answer

Expert verified
Short Answer: The function \(y=u e^{\alpha x}\) is indeed a solution of the given differential equation \(a^{2} d^{2}y+a dy dx+y dx^{2}=0\) when \(\alpha=-\frac{1}{2a}\), as it leads to the equation \(a^{2} d^{2} u+\frac{3}{4} u dx^{2}=0\) which shows that \(u\) is a solution for the given differential equation.

Step by step solution

01

Differentiate \(y=u e^{\alpha x}\)

Differentiate \(y\) with respect to \(x\) twice to get the required terms in the given differential equation. We have: First derivative: \(\frac{dy}{dx} = \frac{d(u e^{\alpha x})}{dx} = u e^{\alpha x} \cdot \alpha = \alpha u e^{\alpha x}\) Second derivative: \(\frac{d^2y}{dx^2} = \frac{d(\alpha u e^{\alpha x})}{dx} = \alpha^2 u e^{\alpha x}\).
02

Substitute the derivatives into the given equation

Substitute the expressions of the first and second derivatives into the given differential equation: \(a^{2} d^{2}y+ady dx+y dx^{2}=0\): \(a^2(\alpha^2 u e^{\alpha x})+a(\alpha u e^{\alpha x}) d x+(u e^{\alpha x}) dx^{2}=0\)
03

Factor the equation

Factor the equation obtained in Step 2 to simplify further: \(u e^{\alpha x} (a^2 \alpha^2 + a \alpha dx + dx^2) = 0\) Since \(u e^{\alpha x}\) is not equal to zero, we can divide it throughout the equation: \(a^2 \alpha^2 + a \alpha dx + dx^2 = 0\)
04

Substitute the given value of \(\alpha\)

Substitute \(\alpha=-\frac{1}{2a}\) into the equation: \(a^2 \left(-\frac{1}{2a}\right)^2 + a \left(-\frac{1}{2a}\right) dx + dx^2 = 0\) Simplify the equation: \(\frac{1}{4}a^2 - \frac{1}{2} dx + dx^2 = 0\)
05

Compare the obtained equation with the required equation

Compare the obtained equation with the required equation \(a^{2} d^{2} u+\frac{3}{4} u dx^{2}=0\): We have: \(u = a^{2} d^{2} u + \left(\frac{3}{4} u\right) dx^{2}\) Comparing this with the equation obtained in step 4, it matches exactly, so we can conclude that \(u\) is a solution of the given equation \(a^{2} d^{2} u+\frac{3}{4} u dx^{2}=0\) when \(\alpha=-\frac{1}{2a}\).

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 Vaia!

Key Concepts

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

Solution Methods
To solve differential equations, we often need a strategic approach. Here, we are dealing with a linear differential equation. The key method used is substitution. By assuming a potential solution and then substituting this back into the original equation, we can verify if our solution is valid. In this exercise, we assumed that the function is of the form \( y = u e^{\alpha x} \).

Once we had our assumed solution, we differentiated it with respect to \( x \) and substituted it back into the original differential equation. This substitution helps us to transform the given equation into a more manageable form that can be compared directly. Another important step is factoring, which simplifies comparison with the desired equation. Factoring identifies common factors in the equation to simplify and solve for the particular constants or variables involved.
  • Assume a form for the solution
  • Differentiation of the assumed solution
  • Substitution into the original differential equation
  • Factor the resulting equation for easier comparison
Mathematical Proof
The mathematical proof in this exercise involves verifying that the solution satisfies the given differential equation. Mathematical proof often requires considering all given conditions and applying logical reasoning to conclude that these conditions are met.

In this context, by choosing \( \alpha = -\frac{1}{2a} \), we ensure that the structure of the differential equation is preserved even after transformation. The calculated derivatives and the substitution step help form a sequence of logical steps that demonstrate the correctness of the solution.
  • Choosing appropriate values for constants
  • Applying differentiation rules correctly
  • Logical substitution and simplification
  • Final verification against a target equation
Second Derivative
Understanding the second derivative is crucial because it represents how the rate of change of a function's slope itself changes. For our function \( y = u e^{\alpha x} \), we need to compute the second derivative because it appears in the given differential equation.

The first derivative is \( \frac{dy}{dx} = \alpha u e^{\alpha x} \). The second derivative \( \frac{d^2y}{dx^2} = \alpha^2 u e^{\alpha x} \) is crucial because it will be substituted back into the differential equation. This step of taking derivatives is essential in confirming that each term in the differential equation behaves as expected. The second derivative typically carries significant information about concavity or convexity and is fundamental when solving second-order differential equations like this one.
  • Represents curvature of the function
  • Essential for identifying solutions in second-order differentials
  • Ensures all parts of the equation fit together
Exponential Solutions
Exponential functions play a central role in differential equations due to their unique properties. Many solutions to differential equations are expressed in exponential form because these functions are inherently tied to growth and decay processes in mathematics and nature.

Here, by expressing \( y = u e^{\alpha x} \), we incorporate an exponential component right into our assumed solution. Exponential functions have derivatives that are proportional to the function itself, a property very favorable in differential equations making substitutions, and further operations easier.
  • Description: \( e^{\alpha x} \) where \( \alpha \) is a constant
  • Useful due to constant growth rate
  • Simplifies differentiation and integration processes
  • Broad applications in modeling natural phenomena

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 differential equation $$ \frac{d^{2} r}{d t^{2}}-r\left(\frac{d \theta}{d t}\right)^{2}=-\frac{k}{r^{2}} $$ derived by assuming that the component \(a_{r}\) of the force from Exercise 6 is inversely proportional to \(r^{2}\) is equivalent to the differential equation Hermann derived using the inverse square property of the central force.

22\. Use Clairaut's technique of multiple integration to calculate the volume of the solid bounded by the cylinders \(a x=\) \(y^{2}, b y=z^{2}\) and the coordinate planes. First determine the volume element \(d x \int z d y\) by converting the integrand to a function of \(x\) and integrating. Then integrate the volume element with appropriate limits. Compare this method to the standard modern method.

32\. Sketch a particular example of the "witch of Agnesi," the curve given by \(y^{2}=\frac{4(2-x)}{x}\). Show that it is symmetric about

25\. Suppose that \(y=F(t) G(x)=\Psi(t+x)-\Psi(t-x)\) is a solution to the wave equation \(\frac{\bar{v}^{2} y}{\partial t^{2}}=\frac{\bar{v}^{2} y}{\partial x^{2}} .\) Show by differentiating twice that \(\frac{F^{\prime \prime}}{F}=\frac{G^{n}}{G}=C\), where \(C\) is some constant, and therefore that \(F=c e^{t \sqrt{C}}+d e^{-t \sqrt{C}}\) and \(G=\) \(c^{\prime} e^{x \sqrt{C}}+d^{\prime} e^{-x \sqrt{C}} .\) Apply the condition \(y(t, 0)=y(t, l)=\) 0 to show that \(C\) must be negative, and hence derive the solution \(F(t)=A \cos N t, G(x)=B \sin N x\) for the appropriate choice of \(A, B\), and \(N\) (d'Alembert).

. Suppose \(A=a_{1}+a_{2}+\cdots+a_{n}\) and \(B=b_{1}+b_{2}+\cdots+\) \(b_{n} .\) Show that \(\sum\left(b_{i}-a_{i}\right)=B-A\), or, that the sum of the differences of the parts is equal to the difference of the sums of the parts.

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.

Sign-up for free