Equipartition 1
The of Energy Theorem.
Annotated lecture notes by M. Croft
---------------------------------------------------------------------------------------------------------------------------Note this material is important to this course and is not in the book. This material applies the
macroscopic concepts of mechanical energy to microscopic collections of ~1023 molecules. In so doing it
casts the concepts of temperature and heat transfer in terms of physics you have already learned.
---------------------------------------------------------------------------------------------------------------------------The equipartition (or equal division) of energy theorem involves the concept that, in thermal
equilibrium, energy is shared equally among all of its various possible forms (or degree of freedom).
Moreover the average amount of energy per degree of freedom is kT/2 per molecule or RT/2 per mole.
[Here k = Boltzmans constant, R= k NA is the ideal gas constant and NA is Avagadros number.]
Operationally a degree of freedom is identified with a quadratic term in the total mechanical energy. For
this class this means a kinetic energy term involving a velocity component squared. {It is worth noting that
it can also be a harmonic oscillator potential energy involving a quadratic displacement from equilibrium
but this concept is not required for 203.}
---------------------------------------------------------------------------------------------------------------------------This figure illustrates the application
of the equipartition principal to a
monatomic ideal gas. Note that there are
three degrees of freedom associated with the
<vx2>, <vy2> and <vz2> kinetic energy terms
respectively. [Here <> denotes the average
taken over all of the molecules of the gas].
By the equal equipartition principal
the internal energy of the ideal monatomic
gas, U, is then N 3 (kT/2), where N is the
number of molecules (atoms here), 3 comes
from 3 degrees of freedom and kT/2 comes
from the energy per degree of freedom
(from the equipartition principal).
The constant volume specific heat
CV= dU/dT|V so that for the ideal
monatomic gas
CV= N 3k/2 per molecule or CV= 3R/2 per
mole. {Technically, for the theoretically
inclined, the derivative is at constant
volume (i.e. |V) and is a partial derivative
(all other variables held constant)}
It is worth noting that if the gas were adsorbed onto a surface, where motion in only two directions
was possible (2 degrees of freedom), that the U would be accordingly reduced.
2
--------------------------------------------------------------------------------------------------------------------This figure illustrates the application
of the equipartition principal to a diatomic
ideal gas. Note that there are now: 3
translational degrees of freedom associated
with the <vx2>, <vy2> and <vz2> ; and 2
rotational degrees of freedom associated
with the <x2>, and <y2>.
{Important aside. Because the atoms are
assumed to be point particles located along
the z-axis, the moment of inertia for
rotations about z is zero and there is no
energy (or degree of freedom) associated
with it. Although the electron cloud extends
a distance from the atoms comparable to
their separation, the mass of the atoms is
located in the nucleus which is many orders
of magnitude smaller so that the point-mass
assumption for the mass distribution is an
excellent approximation.}
Continuing before from the aside,
the equipartition principal dictates the
internal energy of the ideal diatomic gas, U, to be N 5 (kT/2). Here the 5= [3 translational + 2 rotational]
degrees of freedom and all else is as defined before. The CV is obtained, as before, by taking the derivative
of the internal energy and is indicated in the figure.
--------------------------------------------------------------------------------------------------------------------This figure illustrates the application
of the equipartition principal to a polyatomic
ideal gas. Note that there are still 3
translational degrees of freedom associated
with the <vx2>, <vy2> and <vz2>. However
for the polyatomic molecule there are now
the full 3 rotational degrees of freedom
associated with the <x2>, <y2> and <z2>.
The equipartition principal therefore dictates
the internal energy of the ideal polyatomic
gas, U, to be N 6 (kT/2). Here the 6= [3
translational + 3 rotational] degrees of
freedom. The CV is obtained, as before, by
taking the derivative of the internal energy
and is indicated in the figure.
3
--------------------------------------------------------------------------------------------------------------------The table at right indicates the specific
heats of a number of gases. One can see that
the equipartition of energy theorem works
exceedingly well in many cases.
CO2 is in fact a linear molecule and
should have a much smaller CV, however it has
some additional vibrational (bending) degrees
of freedom {NOT REQUIRED FOR THIS
COURSE}. In fact these low lying vibrations
are part of the infrared active modes that make
CO2 a greenhouse gas.
H2O similarly has some bending
vibrations and is also a greenhouse gas.
Diatomic H2 gas shows 3 translational
degrees of freedom at low temperature because
the 2 rotational degrees of freedom freeze out
due to quantum mechanical effects below about
100K. {This concept is not required for this
course but is our first encounter with quantum
mechanics. Basically a quantum system has
discrete allowed energies and the equipartition
principal does not apply. If the average thermal
energy, kT, is small compared to the quantum-allowed energy separation then this degree of freedom
disappears.}
--------------------------------------------------------------------------------------------------------------------NOT REQUIRED FOR 203.
This figure illustrates the temperature
dependence of CV for diatomic H2.
The freezing out of the rotational
degrees of freedom at low temperature
was discussed in the previous slide.
However, at very high temperature one
should note another step increase in
the value of CV. This step occurs
because two additional degrees of
freedom (one kinetic and one
potential) associated with the vibration
of the H-atoms about the molecular
center of mass freeze out due to
quantum mechanical effects below
about 3000K.
4
--------------------------------------------------------------------------------------------------------------------NOT REQUIRED FOR 203. This
figure illustrates the evaluation of CV for a
monatomic solid. Every atom can be
thought of as being bound to a lattice site
like a harmonic oscillator. Thus there are
three kinetic and three potential degrees of
freedom for the vibrations of the atoms
about their equilibrium positions. This
allows one to calculate the internal energy
and specific heat of such a solid and is
known as the law of Dulong and Petit.