Title: Kinetic Theory 2
1Kinetic Theory 2
- Linking Kinetic Theory and Temperature
2Key Ideas
- We are going to relate the rms speed of gas
molecules to the temperature of the gas. - Temperature is a measure of the internal energy
of a material. - The higher the temperature in a gas, the faster
the molecules will travel.
3Some Assumptions
- The internal energy is represented by the
potential energy and kinetic energy in the bonds
of any material. - In a gas, the molecules are so far apart that
there are no intermolecular interactions. So
there is no potential energy. - Therefore the energy is entirely kinetic.
4Kinetic Energy in a Gas
- Kinetic energy is shared randomly throughout the
gas. - This means that any given molecule can be moving
at any velocity. - Because there are lots of molecules, there is a
random distribution of speeds. A few molecules
will travel slowly, a few very fast, while most
will be somewhere in between.
5We can show this on a graph
100 K
1000 K
6Thermal Equilibrium
- If no energy is being transferred as heat between
an object and its surroundings, we say that it is
in thermal equilibrium. - If a gas is in thermal equilibrium and it is not
being compressed or expanded, the average kinetic
energy will remain constant, so will the
temperature.
7Two Relationships from Before
pV nRT and pV 1/3 Nmc2
It does not take a genius to see that nRT 1/3
Nmc2
8Lets look at this relationship further
nRT 1/3 Nmc2
Mean square speed
Mass of each molecule
No of molecules
Total mass of the molecules
It reminds us of the relationship that describes
kinetic energy Ek 1/2 mv2
9So we can write
nRT 2/3 N1/2mc2 since 2/3 1/2 1/3.
Rearranging gives us 1/2mc2 3/2nRT 3/2RT
N N/n
10Since N is the total number of molecules and n is
the number of moles, N/n will always be NA, which
is Avagadros number, 6.02 x 1023. So we can
write 1/2mc2 3/2RT NA
11Boltzmanns Constant
R/NA is called Boltzmanns constant and is given
the code k. We can easily work out the value for
k. k 8.31 1.38 x 10-23 J K-1
6.02 x 1023
And this gives us our final relationship 1/2mc2
3/2kT