Question:Find the steady-state temperature distribution inside a sphere of radius 1 when the surface temperatures are as given in Problems 1 to 10.
35cos4θ.

Short Answer

Expert verified

The steady-state temperature distribution.

ur,θ=8r4P4cosθ+20r2P2cosθ+7P0cosθ.

Step by step solution

01

Given Information.

An expression has been given as 35cos4θ.

02

Definition of Laplace’s equation.

The total of the second-order partial derivatives of , the unknown function, with respect to the Cartesian coordinates equals , according to Laplace's equation.

Laplace’s equation in cylindrical coordinates is

2u=1rr(rur)+1r22uθ2+2uz2=0

And to separate the variable the solution assumed is of the form .

u=R(r)Θ(θ)Z(z)

03

Solve the equation.

Start with the relation mentioned below.

At the boundary , you have

ua,θ=35cos4θ=l=0clPlcosθ

Rewrite the equation by taking,

x=cosθ

ua,θ=35cos4x=l=0clPlx
It is known that a leading term in every Legendre polynomial is of the same order as the polynomial.

Plx=xl+lower order terms

Now, express x4 as belox

x4=P4+

Write the first few Legendre polynomials
P0x=1P1x=xP2x=123x2-1P3x=125x3-3x
P4x=1835x4-30x2+3P5x=1863x5-70x3+15xP6x=116231x6-315x4+105x2-5

04

Rewrite the expression and solve further.

Rewrite the Expression as given by,
35x4=8P4x+30x2-3=8P4x+30x2-3P0x
Express in terms of Legendre polynomials
x2=132P2x+P0x

Therefore, you have,
35x4=8P4x+30132P2x+P0x-3P0x=8P4x+20P2x+7P0x
The boundary condition expressed in terms of Legendre polynomials.
ua,θ=35x4=8P4x+20P2x+7P0x=l=0clPlcosx
See the coefficients where only survive.


Hence, the solution is ur,θ=8r4P4cosθ+20r2P2cosθ+7P0cosθ.

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 Vaia!

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

The velocityof electrons from a high energy accelerator is very near the velocityof light. Given the voltage Vof the accelerator, we often want to calculate the ratio v / c. The relativistic formula for this calculation is (approximately, forV1)

vc=1-(0.511V)2, V=Number of million volts

Use two terms of the binomial series (13.5) to find1 - v/cin terms ofV. Use your result to find 1 - v/cfor the following values of V. Caution: V= the number of millionvolts.

(a) V =100 million volts

(b)V =500 million volts

(c)V =25,000 million volts

(d)V =100 gigavolts (100109 volts105 million volts)

In(2-e-x)

Find a two-term approximation for each of the following integrals and an error bound for the given t interval 0tXe-xdx,0<t<0.01

(a) Using computer or tables (or see Chapter 7,Section 11),verify thatn=1(1/n2)=π26=1.6449=,and also verify that the error in approximating the sum of the series by the first five terms is approximately 0.1813.

(b) By computer or tables verify that n=1(1/n2)(1/2)n=π212-(1/2)(ln2)2=0.5815+

the sum of the first five terms is0.5815+

(c) Prove theorem (14.4). Hint: The error is |N+1anxn|.

Use the fact that the absolute value of a sum is less than or equal to the sum of the absolute values. Then use the fact that |an+1||an|to replace all anby aN+1 , and write the appropriate inequality. Sum the geometric series to get the result.

Derive the formula (1.4) for the sum Snof the geometric progression Sn=a+ar+ar2+.....arn-1.Hint: Multiply Snby rand subtract the result fromSn; then solve for Sn. Show that the geometric series (1.6) converges if and only if r<1; also show that if r<1, the sum is given by equation (1.8).

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.

Sign-up for free