/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q3.17P DeriveP3(x) from the Rodrigues ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

DeriveP3(x)from the Rodrigues formula, and check that P3(cosθ)satisfies the angular equation (3.60) for I=3. Check that P3and P1are orthogonal by explicit integration.

Short Answer

Expert verified

Answer

Hence it is checked using explicit integration that P1xand P3xare orthogonal.

Step by step solution

01

Define functions

Write the formula of Rodrigues’s.

PI(x)=12II!(ddx)I(x2-1)I …… (1)

02

Determine functions

Calculate the P3xusing equation (1).

Therefore,

P3x=1233!ddx3x2-13=148d3dx3x2-13=18d2dx2xx2-12

Solve as further,

P3x=18ddxx2-12+2xx2-12x=18ddxx2-12+4x2x2-1=18ddxx2-12+4x4-4x2=182x2-12x+44x3-8x

Solve as further,

P3x=1820x3-4x-8x=52x3-32x

Therefore,

P3cosθ=52cos3θ-32cosθ

03

Determine that P3(cosθ) satisfies the equation.


1sinθ∂∂θsinθdPdθ=-II+1P

Here, I=3

dP3dθ=ddθ52cos3θ-32cosθ=523cos2θ-sinθ-32-sinθ=-32sinθ5cos2θ-1

Multiply by sinθon both the sides,

sinθdP3dθ=-31sin2θ5cos2θ-1∂∂θsinθdP3dθ=-32∂∂θsin2θ5cos2θ-1=-325cos2θ-12sinθcosθ+sin2θ10cosθ-sinθ=-325cos2θ-cosθ2sinθ-sin3θ10cosθ1sinθ∂∂θsinθ∂P3∂θ=-3225cos3θ-cosθ-10sin2θcosθ=-3×452cos3θ-32cosθ=-II+1P3

1sinθ∂∂θsinθ∂P3∂θ=-3225cos3θ-cosθ-10sin2θcosθ=-3×452cos3θ-32cosθ=-II+1P3

Hence, it is proved.

04

Determine P3 and P1 are orthogonal

Now,

P1x=xP3x=52x3-32x

Using explicit integration the orthogonal condition can be derived as,

∫-1+1P1xP3xdx=0∫-1+1x125x3-3xdx12∫-1+15x4-3x2dx125x55-1+1-3x33-1+1121+1-1=0

Therefore, P1xand P3xare orthogonal.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A stationary electric dipole p⇶Ä=pz^is situated at the origin. A positive

point charge q(mass m) executes circular motion (radius s) at constant speed

in the field of the dipole. Characterize the plane of the orbit. Find the speed, angular momentum and total energy of the charge.

A rectangular pipe, running parallel to the z-axis (from -∞to +∞), has three grounded metal sides, at y=0,y=aand x=0The fourth side, at x=b, is maintained at a specified potential V0(y).

(a) Develop a general formula for the potential inside the pipe.

(b) Find the potential explicitly, for the case V0(y)=V0(a constant).

Charge density

σ(ϕ)=asin(5ϕ)

(whereais a constant) is glued over the surface of an infinite cylinder of radiusR

(Fig. 3.25). Find the potential inside and outside the cylinder. [Use your result from Prob. 3.24.]

In Prob. 2.25, you found the potential on the axis of a uniformly charged disk:

V(r,0)=σ2ε0(r2+R2-r)

(a) Use this, together with the fact that PI(1)=1, to evaluate the first three terms

in the expansion (Eq. 3.72) for the potential of the disk at points off the axis, assuming r>R.

(b) Find the potential for r<Rby the same method, using Eq. 3.66. [Note: You

must break the interior region up into two hemispheres, above and below the

disk. Do not assume the coefficientsAIare the same in both hemispheres.]

A spherical shell of radius carries a uniform surface charge on the "northern" hemisphere and a uniform surface charge on the "southern "hemisphere. Find the potential inside and outside the sphere, calculating the coefficients explicitly up to and .

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.