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Write and solve the Euler equations to make the following integrals stationary. \(\int_{x_{1}}^{x_{2}} \sqrt{x} \sqrt{1+y^{2}} d x\)

Short Answer

Expert verified
Use the Euler-Lagrange equation with the integrand . Solve the resulting differential equation to find y(x).

Step by step solution

01

Identify the functional

The given integral is . Identify the integrand (also known as the functional). In this case, the integrand is .
02

Apply the Euler-Lagrange equation

The Euler-Lagrange equation is given by: . Substitute the functional (x) into this equation.
03

Simplify the Euler-Lagrange equation

Calculate the partial derivatives: . Then, substitute them back into the Euler-Lagrange equation.
04

Solve the resulting differential equation

Once the partial derivatives are substituted into the Euler-Lagrange equation, solve the resulting differential equation to find the function y(x) that makes the integral stationary.

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Key Concepts

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

Euler-Lagrange Equation
The Euler-Lagrange equation is a fundamental equation in the calculus of variations. It helps find functions that extremize (maximize or minimize) functionals. In simpler terms, it is used to determine the path, curve, surface, etc., for which a given integral is stationary (not changing).
This equation is derived from the principle of stationary action. The general form of the Euler-Lagrange equation is:
\[ \frac{d}{dx} \left( \frac{\partial L}{\partial \dot{y}} \right) - \frac{\partial L}{\partial y} = 0 \]
Here, \(L\) is the integrand (also known as the Lagrangian) and depends on \(x\), \(y\), and \(\dot{y} = \frac{dy}{dx}\). The solutions to the Euler-Lagrange equation provide the extremal functions required to make the integral stationary.
Functional
A functional is a map from a space of functions to the real numbers. Think of it as a function, but instead of taking numbers as its inputs, it takes functions as inputs.
In the context of the given problem, the integral we wish to make stationary is a functional:
\[ \int_{x_{1}}^{x_{2}} \sqrt{x} \sqrt{1+y^{2}} \, dx \]
The integrand \(\sqrt{x} \sqrt{1+y^{2}}\) is dependent on both \(x\) and \(y\). Our goal is to find a function \(y = y(x)\) that makes this functional stationary using the Euler-Lagrange equation. The functional tells us how much 'action' is associated with a certain function. The extremal function is what minimizes or maximizes this action.
Differential Equation
A differential equation relates a function to its derivatives. Solving a differential equation means finding a function that satisfies this relationship.
In the last step of solving the Euler-Lagrange equation, we end up with a differential equation. This is because the resulting equation after applying the Euler-Lagrange equation involves derivatives of the function we are trying to find.
For the given problem, after substituting the functional into the Euler-Lagrange equation and simplifying, we obtain a differential equation which needs to be solved to find \(y(x)\), the function that makes the integral stationary. Solving this differential equation is the last critical step in finding the function that optimizes the given integral.

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Most popular questions from this chapter

Write and solve the Euler equations to make the following integrals stationary. \(\int_{x_{1}}^{x_{2}}\left(y^{\prime 2}+y^{2}\right) d x\)

Write and solve the Euler equations to make the following integrals stationary. \(\int_{x_{1}}^{x_{2}}\left(y^{2}+\sqrt{y}\right) d x\)

Write and solve the Euler equations to make the following integrals stationary. Change the independent variable, if needed, to make the Euler equation simpler. \(\int_{0}^{\theta_{2}} \sqrt{r^{\prime 2}+r^{2}} d \theta, \quad r^{\prime}=d r / d \theta\)

Show that if \(F=F\left(x, y, z, y^{\prime}, z^{\prime}\right)\), and we want to find \(y(x)\) and \(z(x)\) to make \(I=\int_{x_{1}}^{x_{2}} F d x\) stationary, then \(y\) and \(z\) should each satisfy an Euler equation as in (5.1). Hint: Construct a formula for a varied path \(Y\) for \(y\) as in Section \(2[Y=y+\epsilon \eta(x)\) with \(\eta(x)\) arbitrary \(]\) and construct a similar formula for \(z\) [let \(Z=z+\epsilon \zeta(x)\), where \(\zeta(x)\) is another arbitrary function]. Carry through the details of differentiating with respect to \(\epsilon\), putting \(\epsilon=0\), and integrating by parts as in Section 2 ; then use the fact that both \(\eta(x)\) and \(\zeta(x)\) are arbitrary to get \((5.1)\)

Find the geodesics on a sphere. Hints: Use spherical coordinates with constant \(r=a\). Choose your integration variable so that you can write a first integral of the Euler equation. For the second integration, make the change of variable \(w=\cot \theta .\) To recognize your result as a great circle, find, in terms of spherical coordinates \(\theta\) and \(\phi\), the equation of intersection of the sphere with a plane through the origin.

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