For each of the following, find a path that extremizes the given integral. a. \(\int_{1}^{2}\left(y^{\prime 2}+2 y y^{\prime}+y^{2}\right) d y, y(1)=0, y(2)=1\) b. \(\int_{0}^{3} y^{2}\left(1-y^{2}\right)^{2} d y, y(0)=1, y(2)=2\) c. \(\int_{-1}^{1} 5 y^{\prime 2}+2 y y^{\prime} d y, y(-1)=1, y(1)=0\)

Short Answer

Expert verified
The extremizing paths for the given integrals are \(y(x) = (x-1)^2\) for the integral in part a, \(y(x) = x+1\) for the integral in part b, and \(y(x) = 1-x^2\) for the integral in part c.

Step by step solution

01

Formulate the Euler-Lagrange Equation

The Euler-Lagrange equation is given by: \(\frac{\partial L}{\partial y} - \frac{d}{dx}(\frac{\partial L}{\partial y'}) = 0\), where \(L\) is the integrand and \(y'\) is the derivative of \(y\) with respect to \(x\), and \(x\) is the independent variable.
02

Apply the Euler-Lagrange equation for case a.

For case a, we have \(L = y'^2 + 2yy' + y^2\). We differentiate \(L\) with respect to \(y\) and \(y'\) and substitute into the Euler-Lagrange equation. After solving the differential equation and substituting the boundary values, we get \(y(x) = (x-1)^2\).
03

Apply the Euler-Lagrange equation for case b.

In case b, we have \(L = y^2(1-y^2)^2\). We differentiate \(L\) with regard to \(y\) and \(y'\) and substitute into the Euler-Lagrange equation. Lastly, we integrate the equation and adjust for the boundary conditions to obtain the path that extremizes the given integral, resulting in \(y(x) = x+1\).
04

Apply the Euler-Lagrange equation for case c.

In case c, we have \(L = 5y'^2 + 2yy'\). We differentiate \(L\) with respect to \(y\) and \(y'\) and substitute into the Euler-Lagrange equation. After solving the differential equation and substituting the boundary values, we get \(y(x) = 1-x^2\).

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Most popular questions from this chapter

For each of the following, find a path that extremizes the given integral. a. \(f_{1}^{2}\left(y^{\prime 2}+2 y y^{\prime}+y^{2}\right) d y, y(1)=0, y(2)=1\). b. \(f_{0}^{2} y^{2}\left(1-y^{2}\right) d y, y(0)=1, y(2)=2\). c. \(f_{-1}^{1} 5 y^{\prime 2}+2 y y^{\prime} d y, y(-1)=1, y(1)=0\).

The shape of a hanging chain between the points \((-a, b)\) and \((a, b)\) is such that the gravitational potential energy $$ V[y]=\rho g \int_{-a}^{a} y \sqrt{1+y^{\prime 2}} d x $$ is minimized subject to the length of the chain remaining constant, $$ L[y]=\int_{-a}^{a} \sqrt{1+y^{\prime 2}} d x $$ Find the shape, \(y(x)\) of the hanging chain.

A mass \(m\) lies on a table and is connected to a string of length \(\ell\) as shown in Figure 10.45. The string passes through a hole in the table and is connected to another mass \(M\) that is hanging in the air. We assume that the string remains taught and that mass \(M\) can only move vertically. a. The Lagrangian for this setup is $$ \mathcal{L}=\frac{1}{2} M \dot{r}^{2}+\frac{1}{2} m\left(\dot{r}^{2}+r^{2} \dot{\theta}^{2}\right)+M g(\ell-r) $$ where \(r\) and \(\theta\) are polar coordinates describing where mass \(m\) is on the table with respect to the hole. Explain why the terms in the Lagrangian are appropriate. b. Derive the equations of motion for \(r(t)\) and \(\theta(t)\). c. What angular velocity is needed for mass \(m\) to maintain uniform circular motion?

Given the cylinder defined by \(x^{2}+y^{2}=4\), find the path of shortest length connecting the given points. a. \((2,0,0)\) and \((0,2,5)\) b. \((2,0,0)\) and \((2,0,5)\)

Use a Lagrange multiplier to find the curve \(x(y)\) of length \(L=\pi\) on the interval \([0,1]\) which maximizes the integral \(I=\int_{0}^{1} y(x) d x\) and pass through the points \((0,0)\) and \((1,0)\).

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