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Questions for Assignment 1 - Physical Chemistry | CHEM 455, Assignments of Physical Chemistry

Material Type: Assignment; Class: PHYSICAL CHEMISTRY; Subject: Chemistry; University: University of Washington - Seattle; Term: Autumn 2005;

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Homework week 1 Chemistry 455A
Wednesday: Q12.3, Q12.4, P12.9, P12.17,
Friday: P12.20, P12.21
Q 1.3/12.3) Why does the analysis of the photoelectric effect based on classical physics
predict that the kinetic energy of electrons will increase with increasing light intensity?
In the classical theory, the energy of the light is the light intensity. So to increase the
light’s energy just focus the light down on a smaller surface. Then the electron that is
ejected must move faster because it was hit with higher energy light.
Classical physicists thought that the greater energy would manifest as a higher speed in
the ejected electron. In fact, the light energy appears as a larger number of electrons
leaving the surface. The kinetic energy of the electrons, surprisingly, is determined by
the photon frequency and the work function of the surface.
Q1.4/12.4) What did Einstein postulate to explain that the kinetic energy of the emitted
electrons in the photoelectric effect depends on the frequency? How does this postulate
differ from the predictions of classical physics?
Einstein postulated that the energy of light depends on the frequency, whereas in
classical theory, the energy depends only on the intensity and is independent of
the frequency. He further postulated that the total energy of light would be a
multiple of hv , and thereby the photon was conceived.
P1.9/P12.9) A newly developed substance that emits 225 W of photons with a
wavelength of 225 nm is mounted in a small rocket such that all of the radiation is
released in the same direction. Because momentum is conserved, the rocket will be
accelerated in the opposite direction. If the total mass of the rocket is 5.25 kg, how fast
will it be traveling at the end of 365 days in the absence of frictional forces?
There is a short way to do this problem: One that shows that the velocity of the rocket
does not depend on the wavelength of the light. The total energy of the light field divided
by the speed of light is the total momentum, which can be equated to the rocket’s
momentum:
()
total total total
rocket
photon
EEE
mv pn p p
Ecpc
== = =
The light leaves with energy, it is not all consumed by the rocket. So you cannot just
equate the energy of the rocket to the energy of the photons that left. But you can
equation the momentum transfer. From Einstein’s famous formula for light:
pf3
pf4
pf5

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Homework week 1 Chemistry 455A

Wednesday: Q12.3, Q12.4, P12.9, P12.17,

Friday: P12.20, P12.

Q 1.3/12.3) Why does the analysis of the photoelectric effect based on classical physics

predict that the kinetic energy of electrons will increase with increasing light intensity?

In the classical theory, the energy of the light is the light intensity. So to increase the

light’s energy just focus the light down on a smaller surface. Then the electron that is

ejected must move faster because it was hit with higher energy light.

Classical physicists thought that the greater energy would manifest as a higher speed in

the ejected electron. In fact, the light energy appears as a larger number of electrons

leaving the surface. The kinetic energy of the electrons, surprisingly, is determined by

the photon frequency and the work function of the surface.

Q1.4/12.4) What did Einstein postulate to explain that the kinetic energy of the emitted

electrons in the photoelectric effect depends on the frequency? How does this postulate

differ from the predictions of classical physics?

Einstein postulated that the energy of light depends on the frequency, whereas in

classical theory, the energy depends only on the intensity and is independent of

the frequency. He further postulated that the total energy of light would be a

multiple of hv , and thereby the photon was conceived.

P1.9/P12.9) A newly developed substance that emits 225 W of photons with a

wavelength of 225 nm is mounted in a small rocket such that all of the radiation is

released in the same direction. Because momentum is conserved, the rocket will be

accelerated in the opposite direction. If the total mass of the rocket is 5.25 kg, how fast

will it be traveling at the end of 365 days in the absence of frictional forces?

There is a short way to do this problem: One that shows that the velocity of the rocket

does not depend on the wavelength of the light. The total energy of the light field divided

by the speed of light is the total momentum, which can be equated to the rocket’s

momentum:

( )

total total total rocket photon

E E E

mv pn p p E cp c

The light leaves with energy, it is not all consumed by the rocket. So you cannot just

equate the energy of the rocket to the energy of the photons that left. But you can

equation the momentum transfer. From Einstein’s famous formula for light:

photon and

total photon

total photon photon

h E cp p

E nE

dE dn Power E n E dt dt

The number of photons per second is given by

1 1 20 1 34 8 1

9

1 J s PowerW W 225J s 2.547 10 s 6.626 10 J s 2.998 10 m s

225 10 m

total

photon

Power n E hc

− − − − −

×

′ = = = = ×

× × ×

×

The momentum of one photon is

34 27 1 9

6.626 10 J s 2.945 10 kg m s 225 10 m

h p

− − − −

×

= = = ×

×

The total number of photons is given from the energy of one photon and total energy:

1 9

27 1 19

28

9

8

86400 s 225 J s 365days =7 10 day

2.945 10 kg m s 8.8 10

Total

photon

Total

photon

Total

Total

E Power Time Joules

E cp Joules

E

n photons E

E

np kgm s c

E v m s c m

− − −

= ⋅ = ⋅ × ⋅

Now equate the momentum of the light beam, with the momentum of the rocket:

( )

28 27 0.8 10 2.945 10

mv (^) rocket np light

v m s m s

  • − = = ⋅ ⋅ ×

For a second way to compute the velocity using the forces:

The force is given by the rate of change of momentum.

( ) (^27 1 20 1 7 ) 2.945 10 kg m s 2.547 10 s 7.501 10 kg ms

d np F n p dt

− − − − − = = ′ = × × × = ×

The final speed is given by

7 2 1 0

7.501 10 kg m s 86400s v v 365days = 4.51m s 5.25 kg day

F

at t m

− − × − = + = = × ×

The total energy of the photon beam is

1 86400s 9 225J s 365days =7 10 day

E Total Power Time Joules

− = ⋅ = ⋅ × ⋅

P12.21 ) The work function of platinum is 5.65 eV. What is the minimum frequency of

light required to observe the photoelectric effect on Pt? If light with a 150-nm wavelength

is absorbed by the surface, what is the velocity of the emitted electrons?

a) For electrons to be emitted, the photon energy must be greater than the work function

of the surface.

19 19

19 15 1 34

1.602×10 J

5.65 eV 9.05 10 J eV

9.05 10 J 1.4 10 s 6.626 10 J s

E h

E

h

− −

− − −

×

×

This photon is in the UV; no wonder Pt is inert.

b) The outgoing electron must first surmount the barrier arising from the work function,

so not all the photon energy is converted to kinetic energy.

2

34 8 1 19 19 9

19 5 1 31

1 2 v

6.626 10 J s 2.998 10 m s 9.05 10 J 4.19 10 J 150 10 m

2 2 4.19 10 J

v = 9.59 10 m s 9.11 10 kg

e

e

e

hc m E h

E

m

− − − − −

− − −

× × ×

= − × = ×

×

× ×

= = ×

×

The energy of the electron is ~2.6eV, compared with 13.6eV for the electron held in the

1s orbital of H.

Monday assigned problems: Q13.3, P13.13, P13.17, P13.

Q13.3) Why can we conclude that the wave function

( ) ( , ) ( )

i E t

ψ x t ψ x e

= represents a

standing wave?

It represents a standing wave because it can be written as the product of a function

that depends only on time with a function that depends only on the spatial

coordinate. Therefore the nodes in ψ (^) ( x )do not move with time.

P13.13) Determine in each of the following cases if the function in the first column is an

eigenfunction of the operator in the second column. If so, what is the eigenvalue?

a) e

− i b 3 x + 2 y g ∂

2

2 x

b) x y

2 2

  • (^) ( )

x y x x

c) sin θ cosθ

2 sin sin 6sin

d d

d d

a) (^) ( )

( 3 2 ) ,

i x y x y e

− + Ψ =

2

2

O ˆ

x

( )

( ) ( )

2 3 2 3 2 2

i x y e i x y O x y e x

− + ∂ − + Ψ = = − ∂

Eigenfunction with eigenvalue –9.

b)

2 2 x + y ( )

x y x x

( )

2 2 1 2 2 x y 2 2 x y x y x x

Eigenfunction with eigenvalue +1.

c) Ψ (^) ( θ ) = sin θ cosθ

sin sin 6 sin

d d O d d

( ) (^) ( )

( ) ( )

3 2 3

2 3

ˆ sin^ cos sin sin 6 sin cos sin sin 1 2 sin 6 sin cos

sin cos 6 sin cos 6 sin cos sin cos 1

d d d O d d d

Eigenfunction with eigenvalue +1.

P13.17) If two operators act on a wave function as indicated by AB f   b g x , it is important

to carry out the operations in succession with the first operation being that nearest to the

function. Mathematically, AB f  ^ (^) b g x (^) = A B f ^ d  (^) b g x iand A ^ f x A A f ^  x

2 b g =^ d b gi. Evaluate the

following successive operations AB f   (^) b g x. The operators A  and B  are listed in the first

two columns and f b g x is listed in the third column.

a)

d

d x

x x e

a x^2

b) x

d

d x

x e

a x^2

c) y x

x y

e

− a x e^2 + y^2 j

Note that your answers to parts (a) and (b) are not identical. As we will learn in Chapter

18, the fact that switching the order of the operators x and d dx changes the outcome of

the operation AB f   (^) b g x is the basis for the Heisenberg uncertainty principle.

a) (^) ( )

2 2 3 2 2 2

d (^) a x a x a x x x e x e a x e d x

 −^  = −^ −