university of kentucky, physics 361 solution to problem set …crawford/phy361_sp10/sol_8e.pdf ·...

University of Kentucky, Physics 361 Solution to Problem Set #8 1. a) The H 2 molecule consists of two hydrogen atoms bound by their shared electrons. The two electron wavefunctions span the entire molecule and have the same spatial wavefunction; therefore they must have opposite spin by the Pauli exclusion principle. However, the protons can be treated like point particles, whose wavefunctions do not overlap, and thus can have any combination of spins. b) The protons has spin s 1 = 1 2 and s 2 = 1 2 . Taking all combinations of m s 1 = ± 1 2 and m s 2 = ± 1 2 : (m s 1 ,m s 2 )=( 1 2 , 1 2 ), ( 1 2 , - 1 2 ), (- 1 2 , 1 2 ), (- 1 2 , - 1 2 ). c) The number of substates listed above is 4. d) To calculate the quantum numbers for ~ S = ~ S 1 + ~ S 2 , the z -component of total spin is S z = S z1 +S z2 or m s ~ = m s 1 ~ + m s 2 ~, so m s =1, 0, 0, -1, respectively, for the above states. The total spin is also quantized: S 2 = ~ 2 s(s + 1), and for each value of s, m s = -s, ..., s in steps of 1. Thus three substates m s =1, 0, -1 belong to s = 1, the triplet, and the remaining state m s = 0 must have s = 0, the singlet. Note: the (s=0,m=0) and (s=1,m=0) states are actually two independent superpositions of the above (m s 1 = 1 2 ,m s 2 = - 1 2 ) and (m s 1 = - 1 2 ,m s 2 = 1 2 ) states. In every case, s 1 = s 2 = 1 2 . Looking at it another way, the total spin quantum number can range from s = |s 1 -s 2 | to s = s 1 +s 2 in steps of one. Thus there are two s-states: s = 1 2 - 1 2 = 0 and s = 1 2 - 1 2 = 1, with the m-substates listed above. e) The m =1, -1 states have m s 1 = m s 2 , or spins aligned, thus the tripet s = 1 states are ortho- hydrogen. Even (s=1,m=0) state behaves as if the spins were aligned. The singlet state s = 0 is the lower energy parahydrogen. The degeneracies of these states are g 1 = 3 and g 0 = 1. f) The number of molecules in each state n i = g i f ( i )= Ag i e - i /kT where A is the normalization constant. Thus n 0 = Ae -0/kT = A and n 1 =3Ae -δ/kT , where δ = 15 meV and the total number of molecules is n = A(1 + 3e -δ/kT ). The fractions or ortho- and para-hydrogen are: f 0 ≡ n 0 n = 1 1+3e -δ/kT and f 1 ≡ n 1 n = 3e -δ/kT 1+3e -δ/kT . g) The average energy is hi = ∑ i i g i f i ∑ i g i f i = 0n 0 + δn 1 n 0 + n 1 = 3δe -δ/kT 1+3e -δ/kT = f 1 δ. 0 25 50 75 100 125 150 175 200 225 250 275 300 0.5 1 f0(T) f1(T) = <E>/δ T (K) 1

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Page 1: University of Kentucky, Physics 361 Solution to Problem Set …crawford/phy361_sp10/sol_8e.pdf · University of Kentucky, Physics 361 Solution to Problem Set #8 1. a) The H 2 molecule

University of Kentucky, Physics 361Solution to Problem Set #8

1. a) The H2 molecule consists of two hydrogen atoms bound by their shared electrons. The twoelectron wavefunctions span the entire molecule and have the same spatial wavefunction; thereforethey must have opposite spin by the Pauli exclusion principle. However, the protons can be treatedlike point particles, whose wavefunctions do not overlap, and thus can have any combination ofspins.

b) The protons has spin s1 = 12 and s2 = 1

2 . Taking all combinations of ms1 = ±12 and ms2 = ±1

2 :(ms1 ,ms2) = (1

2 ,12), (1

2 ,−12), (−1

2 ,12), (−1

2 ,−12).

c) The number of substates listed above is 4.

d) To calculate the quantum numbers for ~S = ~S1+~S2, the z-component of total spin is Sz = Sz1+Sz2or ms~ = ms1~ + ms2~, so ms = 1, 0, 0,−1, respectively, for the above states. The total spin isalso quantized: S2 = ~2s(s + 1), and for each value of s, ms = −s, ..., s in steps of 1. Thus threesubstates ms = 1, 0,−1 belong to s = 1, the triplet, and the remaining state ms = 0 must haves = 0, the singlet. Note: the (s=0,m=0) and (s=1,m=0) states are actually two independentsuperpositions of the above (ms1=

12 ,ms2= − 1

2) and (ms1= − 12 ,ms2=

12) states. In every case,

s1 = s2 = 12 .

Looking at it another way, the total spin quantum number can range from s = |s1−s2| to s = s1+s2in steps of one. Thus there are two s-states: s = 1

2−12 = 0 and s = 1

2−12 = 1, with the m-substates

listed above.

e) The m = 1,−1 states have ms1 = ms2 , or spins aligned, thus the tripet s = 1 states are ortho-hydrogen. Even (s=1,m=0) state behaves as if the spins were aligned. The singlet state s = 0 isthe lower energy parahydrogen. The degeneracies of these states are g1 = 3 and g0 = 1.

f) The number of molecules in each state ni = gif(εi) = Agie−εi/kT where A is the normalization

constant. Thus n0 = Ae−0/kT = A and n1 = 3Ae−δ/kT , where δ = 15 meV and the total numberof molecules is n = A(1 + 3e−δ/kT ). The fractions or ortho- and para-hydrogen are:

f0 ≡n0

11 + 3e−δ/kT

and f1 ≡n1

3e−δ/kT

1 + 3e−δ/kT.

g) The average energy is

〈ε〉 =∑

i εigifi∑i gifi

=0n0 + δn1

n0 + n1=

3δe−δ/kT

1 + 3e−δ/kT= f1δ.