SUBJECT: PHYSICS
CLASS: SS 2
DATE:
TERM: 2nd TERM
WEEK 7
TOPIC: Energy Quantization
Bohr suggested that the electron in the atom exist in discrete energy known as quantizaton which can be removed fom one level to the other. Energy in such bodies is emitted in separate or discrete energy packet called energy quanta (E0
E =hf
H = planckÂs constant.
ENERGY LEVEL IN AN ATOM
Electrons in atoms are arranged around their nuclei in position known as energy level or electron shell. It requires more energy to remove electrons from the first energy level than to remove electrons from any of the other higher levels. The energy of an electron is given by the relation .
E = - 1 R
n2
n = electron quantum number
R = a constant
The minus sign signifies that work must be done on the electron to remove it from the atom.
ENERGY LEVEL DIAGRAM
E n =
E4 n=5
E3 n=
E 2 n =3
E 1 n =2
E o
n = 1 (ground state)
The ground state is the stable state or an atom corresponding to its minimum energy. When an atom is heated with an energetic particle, the atom is excited. An excited state is an allowed state of higher energy when the atom is unstable. One electron volt (IeV)
is the energy acquired by an electron in falling freely through a p.d of 1
Volt = 1.6 x 10 -19J.
During the excitation from lower energy level, the potential energy is converted into Kinetic energy so that the electrons eventually acquire a velocity given by:
The energy gained by electron = charge x p.d = eV. Therefore, the electron moves from one level to the other according to the relation.
En  Eo = hf = eV
λ
Worked example
(a) the frequency of the photon
(b) the wavelength
( C = 3.0 x 108 ms -1, h = 6.625 x 10 -34Js)
â E = En-Eo = 6.2 x 10 -21J
âE = hf
f = âE = 6.2 x 10-21
h 6.625 x 10-34
f = 9.358 x 10 2Hz
But C = f λ
:. λ = C = 3.0 x 108â
f 9.4 x 1012
âE = E2- Eo
= -12.42 x 10-19 – ( -30.3 x 10-19J )
= 17.88 x 10-19J
f = âE = 1.788 x 10-18
h 6.625 x 10-34
f = 2.698 x 1015 Hz.
âE = E2 – EO = -10.3EV – (-26.3ev)
= 16ev
1ev = 1.6 x 10-19 J
:. 16ev = 16 x 1.6 x 10-19J
âE = hf = hc
λ
:.λ = hc = 6.625 x1034 x 3.0 x 108
âE 16 x 1.6 x 10-19
= 1.9875 x 10-25
λ = 7.76 x 10-19 m
KE = ½ mv2 = ev
2ev =mv2
v2 = 2ev
m
But e/m = 1.8 x 1011
V = √2 x 1.5 x 103 x 1.8 x 1011
V = 2.3 x 107m/s
Ke = eV
= 1.6 x 10-19 x 1.5x 103
= 2.4 x 10-16J.
LINE SPECTRA FROM HOT BODIES
If the light of excited gas is examined in a spectrometer, an emission spectrum is seen e.g Neon produces a line spectrum. The spectrum consist of a number of well defined lines, each having a particular wavelength and frequency .
ABSORPTION SPECTRA
Absorption spectra are dark lines in the emission spectrum of a heated substance due to absorption of radiation .Electrons absorb radiation if theyjump from lower energy level to higher energy level.
SPECTRA OF DISCHARGE LAMP
If a gas put into a discharge tube and if its pressure is progressively reduced using a power pump as shown below
When a high p.d is applied at low pressure, an electric discharge takes place in the tube and the gas glows. The gas glows because its atom is given energy by the flow of electricity through the tube. The colour of the gas depends on the nature of the gas used .
Reading Assignment.
New School physics pgs
WEEKend assignment
(A) excited (B) stable (C) ionized
(A)Beta ray (B) Gammar rays (C ) X- rays.
(A)change of electron from a higher to lower energy level
(B) potential energy of the electron inside an atom
(C ) Excitement of an electron in the atom
(A) atoms (B)ions (C ) electrons
(A ) 146 (B) 330 (C ) 73.
Theory
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