1-27 Quantization of Energy
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Transcript of 1-27 Quantization of Energy
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Quantization of Energy
ABELLA / BASCUNA / RAVELO // IV - TRUTH
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ULTRAVIOLET CATASTROPHE RAYLEIGH-JEANS LAW:
As l approaches zero, the function I approaches infinity.
Hence, according to classical theory, not only should short
wavelengths predominate in a blackbody spectrum, but also
the energy emitted by any black body should become
infinite in the limit of zero wavelength.
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ULTRAVIOLET CATASTROPHE
In contrast to this prediction, the
experimental data plotted in Figure
40.5 show that as wavelength
approaches zero, intensity also
approaches zero. This mismatch of
theory and experiment was so
disconcerting that scientists called it
the ultraviolet catastrophe.
Note: This “catastrophe”— infinite energy—occurs as the
wavelength approaches zero; the word ultraviolet was
applied because ultraviolet wavelengths are short.
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ULTRAVIOLET CATASTROPHE The Ultraviolet catastrophe is the error
at short wavelengths in the Rayleigh–
Jeans law known as the “classical
theory” for the energy emitted by an
ideal black-body. The error, much more
pronounced for short wavelengths, is
the difference between the blue curve
(Rayleigh–Jeans law) and the red curve
(Planck's law).
BASICALLY:
At long wavelengths, the Rayleigh–
Jeans law is in reasonable agreement
with experimental data, but at short
wavelengths, major disagreement is
apparent.
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MAX PLANCK’S SOLUTION
Planck assumed the cavity radiation
came from atomic oscillators in the
cavity walls of a blackbody (a
hypothetical object capable of
absorbing all the electromagnetic
radiation falling on it).
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MAX PLANCK’S SOLUTION
TWO MAJOR ASSUMPTIONS OF MAX PLANCK 1. The energy of an oscillator can have only certain discrete values
En
En = nhf n = positive number called quantum number f = frequency of the oscillator
h = Planck’s constant
Since energy can only have discrete values En, we say that energy
is quantized.
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MAX PLANCK’S SOLUTION
TWO MAJOR ASSUMPTIONS OF MAX PLANCK 2. The oscillators emit or absorb energy when making a transition
from one quantum state to another.
The amount of energy emitted by the oscillator and carried by the
quantum of radiation is given by E = hf
An oscillator emits or absorbs energy only when it changes quantum states. If it remains in one quantum state, no energy is
absorbed or emitted.
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MAX PLANCK’S SOLUTION This is an energy-level diagram
showing the quantized energy levels
and allowed transitions proposed by
Planck.
The major point of Planck’s theory is
the assumption of quantized energy
states which led to the birth of
quantum theory – a clear deviation
from the classical theory.
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MAX PLANCK’S SOLUTION
HIGH FREQUENCIES (short WAVELENGTHS) LOW FREQUENCIES (HIGH WAVELENGTHS)
Energy levels are far apart Energy levels are close together
Large energy for each transition Small energy for each transition
Boltzmann factor is small Boltzmann factor is large
Relatively less energy states are excited Many energy states are excited
Large energy per transition but less excited states = low intensity
Many excited states but small energy per transition = low intensity
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MAX PLANCK’S SOLUTION
Max Planck then generated a theoretical expression which
matched the experimental curve at all given wavelengths.
Planck’s constant (h) was derived experimentally. First he
assumed that light behaved like particles which had
energy hf with f as the frequency and h as the constant.
Then through experimentation using a vacuum tube. He
then excited electrons in the cathode with a lightsource of
known wavelength and measured the energy across the
tube. Given f and E he was able to derive the value for h.
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APPLICATIONS