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(a) Plugs=0,s=2, and s=3into Kramers' relation (Equation 6.104) to obtain formulas for (r-1),(r),(r-2),and(r3). Note that you could continue indefinitely, to find any positive power.

(b) In the other direction, however, you hit a snag. Put in s=-1, and show that all you get is a relation between role="math" localid="1658216018740" (r-2)and(r-3).

(c) But if you can get (r-2)by some other means, you can apply the Kramers' relation to obtain the rest of the negative powers. Use Equation 6.56(which is derived in Problem 6.33) to determine (r-3) , and check your answer against Equation 6.64.

Short Answer

Expert verified

(a)The Kramer's relation value of

s=1r=a2[3n2-l(l+1)]s=2r2=n2a22[5n2-3l(l+1)+1]s=3r3=n2a38[35n4+25n2-30n2l(l+1)+3l2(l+1)2-6l(l+1)]

(b) The value of s=-1is r-3=1al(l+1)r2

(c) The value of r-3is 1a3n3II+1I+12

Step by step solution

01

Given information

The values of to be substituted in the Kramer’s relation are 0,1,2,3.

1r2=1(l+1/2)n3a2. . . . . . . 6.56

02

Determine the formula for Kramer's relation

When computing, in particular, perturbative corrections to the hydrogen spectrum, the Kramer’s relationship is crucial since those calculations call for expectation values of the radial Hamiltonian.

It gives the expectation values of close powers of r for the hydrogen atom.

s+1n2(rs)-(2s+1)ars-1+s4(2l+1)2-s2a2r(s-2)=0.

03

Solve the s=0,  s=1,  s=2 and s=3 into Kramer’s' relation

a)

Several values for s must be inserted into Kramer's relation.

s=0

1n2-ar-1=0r-1=1an2

For s=1,

2n2r-3a+14(2l+1)2-1a2r-1=0r=n22a24r-1(-4l2-4l)+3a=n22-a21an2l(l+1)+3ar=a2[3n2-l(l+1)]

Also for s=2 ,

3n2r2-5ar+12(2l+1)2-4a2=0

r2=n235ar+a224l2+4l-3=n235a223n2-l2-l-a224l2+4l-3=n2a2615n2-9l2-9l+3r2=n2a265n2-3ll+1+1

Lastly, for s=3,

4n2r3-7ar2+34(2l+1)2-9a2r=0

r3=n247ar2-3a244l2+4l-8r=n247an2a225n2-3li+1+1-3a2ll+1-2a23n2-ll+1=n2a2835n4-21n2ll+1+7n2-9n2ll+1+3l2l+12+18n2-6ll+1nr3=n2a2835n4+25n2-30n2ll+1+3l2l+12-6ll+1

04

Step 4: Show that for s=-1 relation between (r-2) and (r-3)

(b)

In Kramer's relation, substitute s=-1,

ar2-142l+1-1a2r-3=0r-3=1all+1r-2

Thus, for the value of s= -1 , the obtained result is a relation between r-3and r-2.

05

Step 5: Determine (r-3)

c)

Evaluate from r-2from the previous step,

r-2=1a2n2l+12r-3=1all+11a2n2l+12=1a3n3ll+1l+12

Therefore, the value of r-3is 1a3n3ll+1l+12.

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Most popular questions from this chapter

For the harmonic oscillator[Vx=1/2kx2], the allowed energies areEN=(n+1/2)ħω,(n=0.1.2,..),whererole="math" localid="1656044150836" ω=k/mis the classical frequency. Now suppose the spring constant increases slightly:k(1+ο')k(Perhaps we cool the spring, so it becomes less flexible.)

(a) Find the exact new energies (trivial, in this case). Expand your formula as a power series inο,, up to second order.

(b) Now calculate the first-order perturbation in the energy, using Equation 6.9. What ishere? Compare your result with part (a).

Hint: It is not necessary - in fact, it is not permitted - to calculate a single integral in doing this problem.

Question: In Problem 4.43you calculated the expectation value ofrsin the stateψ321. Check your answer for the special cases s = 0(trivial), s = -1(Equation 6.55), s = -2(Equation 6.56), and s = -3(Equation 6.64). Comment on the case s = -7.

Consider the (eight) n=2states, |2ljmj. Find the energy of each state, under weak-field Zeeman splitting, and construct a diagram like Figure 6.11 to show how the energies evolve asBext increases. Label each line clearly, and indicate its slope.

Question: Evaluate the following commutators :

a)[L·S,L]

b)[L·S,S]

c)role="math" localid="1658226147021" [L·S,J]

d)[L·S,L2]

e)[L·S,S2]

f)[L·S,J2]

Hint: L and S satisfy the fundamental commutation relations for angular momentum (Equations 4.99 and 4.134 ), but they commute with each other.

[LX,LY]=ihLz;[Ly,Lz]=ihLx;[Lz,Lx]=ihLy.......4.99[SX,SY]=ihSz;[Sy,Sz]=ihSx;[Sz,Sx]=ihSy........4.134

Estimate the correction to the ground state energy of hydrogen due to the finite size of the nucleus. Treat the proton as a uniformly charged spherical shell of radius b, so the potential energy of an electron inside the shell is constant:-e2/(4πϵ0b);this isn't very realistic, but it is the simplest model, and it will give us the right order of magnitude. Expand your result in powers of the small parameter, (b / a) whereis the Bohr radius, and keep only the leading term, so your final answer takes the form ΔEE=A(b/a)n. Your business is to determine the constant Aand the power n. Finally, put in b10-15m(roughly the radius of the proton) and work out the actual number. How does it compare with fine structure and hyperfine structure?

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