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Write theθLagrange equation for a particle moving in a plane ifV=V(r) (that

is, a central force). Use theθequation to show that:

(a) The angular momentum r×mvis constant.

(b) The vector r sweeps out equal areas in equal times (Kepler’s second law).

Short Answer

Expert verified

Part a and b are verified.

Step by step solution

01

Definition of Kepler's Second law

Kepler's second law of planetary motion describes the speed of a planet traveling in an elliptical orbit around the Sun. It states that a line between the Sun and the planet sweeps equal areas at equal times.

02

Given Parameters

It is given that the Lagrange equation for a particle moving in a plane if

V=V(r)(Central force).

03

Show that the angular momentum r × mv is constant

Now Lagrangian for a particle moving in a plane is

L=12mv2-Vrv=rr^+rθ^......(1)L=12mr2+r2θ2-Vr......(2)

Whereandare unit vectors in r and θ direction respectively.

Now applying the Euler-Lagrange equation to (2) in the θ direction yields as

Lθ=mr2θLθ=0......(3)Lθ=Lθmr2θ=constant.....(4)

Now to show that equation (3) is the z component of angular momentum,

Lz=mr×vz......(5)r×v=rr^×rr^+rθθ^r×v=rr×r^+r2θr^×θ^r^×r^=0r^×θ^=z^r×vz=r2θLz=mr2θ

By comparing equation (5) with (3) it shows that the angular momentum is constant.

04

Show that the vector r sweeps out equal areas in equal times (Kepler’s second law)

A figure below show that the differential area and displacement are related by

dA=12r×drzdA=12r×vzdt......(10)A=12r×vz

Angular momentum is constant therefore is constant. By transitive property

Hence, this is Kepler's second law.

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Most popular questions from this chapter

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

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

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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.

A hoop of mass m in a vertical plane rests on a frictionless table. A thread is wound many times around the circumference of the hoop. The free end of the thread extends from the bottom of the hoop along the table, passes over a pulley (assumed weightless), and then hangs straight down with a mass m (equal to the mass of the hoop) attached to the end of the thread. Let xbe the length of thread between the bottom of the hoop and the pulley, letybe the length of thread between the pulley and the hanging mass, and letθbe the angle of rotation of the hoop about its center if the thread unwinds. What is the relation betweenx,y, andθ? Find the Lagrangian and Lagrange’s equations for the system. If the system starts from rest, how does the hoop move?

(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.

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