Section 16.4

The Hamilton--Jacobi Equation

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Problem 6011

Find the field function p(x,y)p(x,y) and the field of extremals itself, passing through the origin, of the integral

∫(0,0)(x,y)1+y′2y dx,y>0. \int _{(0,0)}^{(x,y)} \frac{\sqrt{1+y'^{2}}}{y} \, dx, \quad y > 0.
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Problem 6012

It is given that a family of extremals passes through the point (x0,y0)(x_{0},y_{0}). Denoting by (x1,y1)(x_{1},y_{1}) the point of intersection of these extremals with some transversal, show that the integral

∫(x0,y0)(x1,y1)f(x,y,y′) dx \int _{(x_{0},y_{0})}^{(x_{1},y_{1})} f(x,y,y') \, dx

taken along the extremal has a constant value.

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Problem 6013

A one-parameter family of extremals is intersected by two transversals. Prove that the integral ∫f(x,y,y′) dx\int f(x,y,y') \, dx, taken along any extremal between the points of intersection with the transversals, has a constant value.

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Problem 6014

Among the lines joining the line x=0x=0 with the point A(x1,y1)A(x_{1},y_{1}), where x1>0x_{1} > 0, y1>0y_{1} > 0, find the one that gives the minimum of the integral

∫0x1+y′2y dx,y>0. \int _{0}^{x} \frac{\sqrt{1+y'^{2}}}{y} \, dx, \quad y > 0.

Also form the Hamilton--Jacobi equation and find the equidistant curves for the extremals transversally intersecting the line x=0x=0.

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Problem 6015

Find the Hamilton--Jacobi equation and the transversals for the field of extremals y=axy=ax of the integral ∫y′2 dx\int y'^{2} \, dx.

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Problem 6016

Find the transversals for the field of extremals y=axy=ax of the integral

I=∫G(y′) dx. I = \int G(y') \, dx.
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Problem 6017

Find the transversals for the field of extremals y=x+ay=x+a of the integral

I=∫(xy′4−2yy′3) dx. I = \int (xy'^{4} - 2yy'^{3}) \, dx.
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Problem 6018

Find the transversals for the field of extremals y=x−x2ay = x - \frac{x^{2}}{a} of the integral

∫y(1−y′2) dx,a>0, x>0; y>0. \int \sqrt{y(1-y'^{2})} \, dx, \quad a > 0, \ x > 0; \ y > 0.
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Problem 6019

Find the extremals of the integral

I=∫M1M2G(y)1+y′2 dx I = \int _{M_{1}}^{M_{2}} G(y)\sqrt{1+y'^{2}} \, dx

by solving the Hamilton--Jacobi equation, and conversely --- find the solution of the Hamilton--Jacobi equation, starting from the first integral of Euler's equation.

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Problem 6020

Find the extremals of the integral

I=∫x0x1x2+y21+y′2 dx I = \int _{x_{0}}^{x_{1}} \sqrt{x^{2}+y^{2}} \sqrt{1+y'^{2}} \, dx

by means of solving the Hamilton--Jacobi equation.

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Problem 6021

Knowing that the paths of light rays are curves along which light propagates in the shortest time, and knowing that the speed of light is inversely proportional to the refractive index of the medium nn, show that the brachistochrone (problem 5989) is the path of light in a medium in which the refractive index nn is expressed by the formula

n=12gy. n = \frac{1}{\sqrt{2gy}}.

In connection with this, find the paths of light rays in such a medium and the equation of the wave surfaces. For the brachistochrones, find the synchrones, i.e., the curves reached simultaneously by points moving from the point (0,0)(0,0) along different brachistochrones.

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Problem 6022

Find the trajectory of a material point moving under the influence of gravity, starting from the principle of least action, according to which for the trajectory of the point the first variation of the "action" integral vanishes:

I=∫2(U+h) ds. I = \int \sqrt{2(U+h)} \, ds.

Here UU is the potential; in this case U=−gyU = -gy, if the axis OYOY is directed upward.

Form the Hamilton--Jacobi equation and, having solved it, find the extremals, in particular those passing through the origin. Investigate the character of the minimum of the integral.

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Problem 6023

Find the trajectory for the motion of a point in a plane under the action of a repulsive force from the axis OXOX, proportional to the distance of the point from this line and directed parallel to the axis OYOY, under the condition that the energy integral has the form v22−y22=0\frac{v^{2}}{2} - \frac{y^{2}}{2} = 0, starting from the "action" integral

I=∫x0x1y1+y′2 dx,y>0. I = \int _{x_{0}}^{x_{1}} y\sqrt{1+y'^{2}} \, dx, \quad y > 0.
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Problem 6024

A material point describes the circle r=2Rcos⁡θr = 2R\cos \theta (in polar coordinates rr and θ\theta) of radius RR under the action of a central force kr5\frac{k}{r^{5}}, inversely proportional to the fifth power of the distance from the center of force, lying at the origin. Show that the "action" integral, taken along any arc of this circle: −π2<θ1≤θ≤θ2<π2-\frac{\pi }{2} < \theta_{1} \leq \theta \leq \theta_{2} < \frac{\pi }{2}, is a strong minimum.

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Problem 6025

Study the motion of a material point under the action of a central force proportional to the distance from the center OO of the force, starting from the principle of least action and applying the Jacobi--Hamilton method.

Show that at the conjugate critical points of any trajectory of the point, regarded as an extremal of the "action" integral, the tangents are mutually perpendicular.

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Problem 6026

Solving the Hamilton--Jacobi equation, find the geodesic lines on a Liouville surface, for which the line element has the form

ds2=(f(x)+g(y))(dx2+dy2). ds^{2} = (f(x)+g(y))(dx^{2}+dy^{2}).
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Problem 6027

Prove that for surfaces whose line element is determined by the equality

ds2=E(u,v) du2+2F(u,v) du dv+G(u,v) dv2, ds^{2} = E(u,v) \, du^{2} + 2F(u,v) \, du \, dv + G(u,v) \, dv^{2},

the Jacobi--Hamilton equation for the problem of the geodesic line has the form

G(∂w∂u)2−2F∂w∂u∂w∂v+E(∂w∂v)2=EG−F2. G\left(\frac{\partial w}{\partial u}\right)^{2} - 2F\frac{\partial w}{\partial u}\frac{\partial w}{\partial v} + E\left(\frac{\partial w}{\partial v}\right)^{2} = EG - F^{2}.
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Problem 6028

Find the shortest distance between a given point and the parabola y2=2pxy^{2} = 2px.

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Problem 6029

Find the minimum of the integral

∫01(12y′2+yy′+y′+y) dx, \int _{0}^{1} \left(\frac{1}{2}y'^{2} + yy' + y' + y\right) \, dx,

if the values at the endpoints of the interval are not given.

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Problem 6030

Find the shortest distance between two circles C1C_{1} and C2C_{2}, lying in one plane.

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Problem 6031

For the problem of finding the minimum of the integral

I=∫f(x,y,y′) dx I = \int f(x,y,y') \, dx

the Hamilton--Jacobi equation is given: wx=H(x,y,wy)w_{x} = H(x,y,w_{y}). Find the function f(x,y,y′)f(x,y,y').

Example. (∂w∂x)2+(∂w∂y)2=1\left(\frac{\partial w}{\partial x}\right)^{2} + \left(\frac{\partial w}{\partial y}\right)^{2} = 1.

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Problem 6032

The Hamilton--Jacobi equation for the problem of the minimum of the integral ∫f(x,y,y′) dx\int f(x,y,y') \, dx has the form

(∂w∂x)2+(∂w∂y)2=x2+y2. \left(\frac{\partial w}{\partial x}\right)^{2} + \left(\frac{\partial w}{\partial y}\right)^{2} = x^{2}+y^{2}.

Find the function f(x,y,y′)f(x,y,y').

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