Use Fermat’s principle to find the path followed by a light ray if the index of refraction is proportional to the given function

11.x+1

Short Answer

Expert verified

y=Clnx+12-C2+x+1+B, whereB is the integration constant.

Step by step solution

01

Given Information.

The givenfunctionisx+1.Path followed by light is to be found out using Euler equations.

02

Definition of Euler equation

In the calculus of variations andclassical mechanics, the Euler equations is a system of second-orderordinary differential equations whose solutions arestationary points of the givenaction functional.

03

Use Euler equation

To find the path traversed by light in a given medium, the path taken by the light is to be minimized(time wise). Velocity of light is scaled by a factor n-1in a refractive medium, then the time required to travel from point A to point B is

t=ABdt=ABvds=c-1ABnds

Therefore, following integral needs to be minimized

nds=ndx2+dy2=n1+y'2dx

Here n=x+1

ThereforeF=x+11+y'2is to be minimized

Euler equation for coordinatesx,yis ddxFy'-Fy=0

Calculate the required derivatives

Fy'=x+1y'1+y'2Fy=0

Therefore,

ddxx+1y'1+y'2=0x+1y'1+y'2=C

WhereCis constant.

Square both sides of the equation to gety'

x+12y'2=C21+y'2x+12-C2y'2=C2y'=Cx+12-C2

Integratey'=Cx+12-C2to gety

y=Cx+12-C2dx=Clnx+12-C2+x+1+B

Therefore, y=Clnx+12-C2+x+1+B , whereB is integration constant.

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Most popular questions from this chapter

(a) Consider the case of two dependent variables. Show that if F=F(x,y,z,y',z')and we want to find y(x)and z(x)to make I=x1x2Fdxstationary, then yand zshould each satisfy an Euler equation as in (5.1). Hint: Construct a formula for a varied path Yfor yas in Section 2 [Y=y+εη(x)with η(x)arbitrary] and construct a similar formula for z[let Z=z+εζ(x), where ζ(x)is another arbitrary function]. Carry through the details of differentiating with respect to ε, putting ε=0, and integrating by parts as in Section 2; then use the fact that both η(x)and ζ(x)are arbitrary to get (5.1).

(b) Consider the case of two independent variables. You want to find the function u(x,y)which makes stationary the double integral y1y2x1x2F(u,x,y,ux,uy)dxdy.Hint: Let the varied U(x,y)=u(x,y)+εη(x,y)where η(x,y)=0at x=x1,x=x2,y=y1,y=y2but is otherwise arbitrary. As in Section 2, differentiate with respect to ε, ε=0set ε=0, integrate by parts, and use the fact that ηis arbitrary. Show that the Euler equation is then xFux+yFuy-Fu=0.

(c) Consider the case in which Fdepends on x,y,y'and y''. Assuming zero values of the variation η(x)and its derivative at the endpoints x1and x2, show that then the Euler equation becomesd2dx2Fy''-ddxFy'+Fy=0.

Show that the actual path is not necessarily one of minimum time. Hint: In the diagram, A is a source of light; CD is a cross section of a reflecting surface, and B is a point to which a light ray is to be reflected. APB is to be the actual path and AP'B, AP"B represent varied paths. Then show that the varied paths:

(a) Are the same length as the actual path if CD is an ellipse with A and B as foci.

(b) Are longer than the actual path if CD is a line tangent at P to the ellipse in (a).

(c) Are shorter than the actual path if CD is an arc of a curve tangent to the ellipse at P and lying inside it. Note that in this case the time is a maximum!

(d) Are longer on one side and shorter on the other if CD crosses the ellipse at P but is tangent to it (that is, CD has a point of inflection at P).

Find a first integral of the Euler equation for the Problem if the length of the wire is given.

Find the geodesics on the cone x2+y2=z2. Hint: Use cylindrical coordinates.

The speed of light in a medium of index of refraction n is v=dsdt=cn. Then the time of transit from AtoBis t=ABdt=c-1ABnds. By Fermat’s principle above, t is stationary. If the path consists of two straight line segments with n constant over each segment, then

ABnds=n1d1+n2d2,

and the problem can be done by ordinary calculus. Thus solve the following problems:

1. Derive the optical law of reflection. Hint: Let light go from the point A=(x1,y1)to B=(x2,y2)via an arbitrary point P=(x,0)on a mirror along thex-axis. Setdtdx=(nc)dDdx=0, where D=distanceAPB, and show that then θ=ϕ.

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