104 2 Quantum Mechanics – I
2.9 In atomic physics the atomic units are as follows:
(i) (a) The Bohr radius^2 /mee^2 is used as the unit of length. (b) The energy
is measured in multiples of the ionization energy of hydrogenmee^2 / 2 ^2
(c)^2 =1(d)e^2 = 2
(ii) In atomic units the Schrodinger equation
−
^2
2 me
∇^2 u−
e^2 u
r
=Eu
would read as
−∇^2 u−
2 u
r
=Eu
2.10 (a) Let the separation between the two nuclei each of chargeqbe 2d, then the
negative chargeQon the electrons is at a distancedfrom either nuclei
Total potential energy due to electrostatic interaction between three objects
is
qQ
d
+
qQ
d
+
q^2
2 d
≤ 0
Taking the equality sign and cancellingq
Q=−
q
4
(b) LetT 0 be the initial kinetic energy andp 0 the momentum of the ion andT
the kinetic energy andpthe momentum of the composite molecule andQ
the excitation energy.
T 0 =T+Q Energy conservation (1)
p 0 =p Momentum conservation (2)
∴(2mT 0 )^1 /^2 =(2. 2 mT)^1 /^2 (3)
The mass of the composite being 2mas the excitation energy is expected
to be negligible in comparison with the mass of the molecule. From (3) we
get
T=
T 0
2
(4)
Using (4) in (1), we findQ=T 20 =^10
− 19
2 =^5 ×^10
− (^20) J
2.11(a) Stationary orbits will be such that the circumference of a circular orbit is
equal to an integral number of deBroglie wavelength so that constructive
interference may take place i.e. 2πr=nλ
Butλ=h/p
∴L=rp=nh/ 2 π (Bohr’s quantization condition) (1)