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).

Short Answer

Expert verified

Answer

By geometric construction, we have to prove that:

a) An ellipse is for any point P on the ellipse sum of distances to the two foci A and B is constant (i.e.PA+PB=2a).

b)AP+PBAP'+P'B

c)AP+PBAP'+P'B

d) Depending on where P' is, AP+PBcan be less than or more thanAp'+P'B.

Step by step solution

01

Given Information.

In the given 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.

02

Definition of light reflection.

When a ray of light strikes a smooth polished surface and bounces back, this is referred to as a light reflection. The incident light ray is said to be reflected off the surface when it lands on it. The reflected ray is the ray that rebounds back.

03

Show that the actual path is not necessarily one of minimum time.

One of the features of an ellipse is that the total of distances to the foci A and B is constant for any point P on the ellipse, (i.e.PA+PB=2a). Therefore,PA+PB=P'A+P'BP'A+P'B=P"A+P"B......(1)

A) By geometric construction in the figure below, it is obvious that:AP+PBAP'+P'B.

B) Once again, proof is obtained using geometric construction. Because the curve CD is tangent to the ellipse and the inside of the ellipse's perimeter, the time situation is inverted. The following is taken from the diagram: AP+PBAP'+P'B.

C) The proof is shown in the diagram below. AP+PBcan be less than or greater than AP+PB, depending on where P' isAP+PB.

Hence, proved.

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Most popular questions from this chapter

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.

In Problems 5 to 7, use Fermat’s principle to find the path followed by a light ray if the index of refraction is proportional to the given function.

(2x+5)12.

For small vibrations, find the characteristic frequencies and the characteristic modes of vibration of the coupled pendulums shown. All motion takes place in a single vertical plane. Assume the spring is unstretched when both pendulums hang vertically and take the spring constant ask=mg/lto simplify the algebra. Hints: Write the kinetic and potential energies in terms of the rectangular coordinates of the masses relative to their positions hanging at rest. Don’t forget the gravitational potential energies. Then write the rectangular coordinates xand yin terms of θand ϕ, and for small vibrations approximate sinθ=θ,cosθ=1-θ2/2, and similar equations for ϕ.

A simple pendulum (Problem 4) is suspended from a mass Mwhich is free to movewithout friction along the xaxis. The pendulum swings in thexyplane and gravityacts in the negativezdirection. Find the Lagrangian and Lagrange’s equations forthe system.

Set up Lagrange’s equations in cylindrical coordinates for a particle of mass min a potential field V(r,θ,z). Hint: v=dsdt; writein cylindrical coordinates.

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