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(or life as a molecule)

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Title: (or life as a molecule)


1
Kinetic Theory
  • (or life as a molecule)

2
Objective
  • Be able to define temperature and pressure
  • Be able to perform simple calculations using the
    Ideal Gas Law

3
Reading
  • Wallace and Hobbs, pp. 64, 74
  • Bohren and Albrecht
  • pp. 1-30

4
Kinetic Theory
  • Once Upon A Time There Was A Molecule

5
Kinetic Theory
  • The molecule had no size or internal structure,
    but it was a happy molecule. Her name was Point
    Mass.

m mass
6
Kinetic Theory
  • One day, Point Mass decided to move. He only
    moved in one direction. He moved a a constant
    speed.

x - direction
velocity vx
7
Kinetic Theory
  • He had momentum!

momemtum mvx
x - direction
velocity vx
8
Kinetic Theory
  • He had so much momentum, he could not slow down
    when he saw the wall!

9
Kinetic Theory
  • He hit the wall!

OUCH!
Area A
x
x
10
Kinetic Theory
  • But much to his surprise, he rebounded! His
    collision was perfectly elastic! No energy was
    lost in the collision.

11
Kinetic Theory
  • He had the same momentum leaving the wall as he
    had before the collision, but in the opposite
    direction.

momentum
12
Kinetic Theory
  • His change in momentum was

Change in Momentum
13
Kinetic Theory
  • The force exerted on Point Mass by the wall was

or
14
Kinetic Theory
  • Point Mass had other friends who are molecules
    identical to himself.

15
Kinetic Theory
  • They all move at the same velocity vx

16
Kinetic Theory
  • The molecules do not interact between themselves
    ...

17
Kinetic Theory
  • but they all interacted with the wall

18
Kinetic Theory
  • The number of molecules (N) in a given volume (V)
    is the number density (n)

V Volume
N of molecules
n number density
19
Kinetic Theory
  • The flux of molecules headed toward the wall is
    ...

vx
1/2 moving towards at vx
1/2 moving away at vx
vx
20
Kinetic Theory
  • The number of molecules striking the wall (A)
    during a time period (t) is ...

A
vx
vx
t
21
Kinetic Theory
  • The total time integrated force on the wall (A)
    is ...

A
22
Kinetic Theory
  • The time-averaged force on the wall is ...

A
23
Kinetic Theory
  • The average force per unit area is ...

A
24
Kinetic Theory
  • Which is pressure!

A
25
Kinetic Theory
  • Lets modify one assumption. The molecules are
    moving at different speeds.

26
Kinetic Theory
  • Lets replace vx2 with an average.

27
Kinetic Theory
  • In reality, the molecules are moving in all
    directions (not just x).

28
Kinetic Theory
  • Substitute back into the equation

29
Kinetic Theory
  • This looks like Kinetic Energy!

Monatomic Gas
KE
30
Kinetic Theory
  • Definition of Temperature
  • Temperature is a measure of the average KE of the
    molecules!

where k Boltzmann Constant 1.38
x 10-23 J/K
31
Kinetic Theory
  • Substitute temperature into pressure

32
Kinetic Theory
  • Ideal Gas Law

where ... p pressure V volume N number of
molecules T temperature k Boltzman Constant
or
33
Kinetic Theory
  • Monatomic Molecules
  • Energy Is a Result of Atoms Motion Only

34
Kinetic Theory
  • Polyatomic Molecules
  • Energy Is a Result of
  • Atoms Motion
  • Rotation, Vibration and Oscillation of Molecule

35
Kinetic Theory
  • Polyatomic Molecules
  • Need to Account for Other Forms of Molecular
    Energy

36
Kinetic Theory
  • Polyatomic Molecules
  • More Complex Molecules Have More Rotational
    Vibrational Energy

37
Kinetic Theory
  • Polyatomic Molecules
  • More Complex Molecules Have More Rotational
    Vibrational Energy

38
Kinetic Theory
  • Polyatomic Molecules
  • Low Pressure
  • Approximates Ideal Gas
  • High Pressure
  • Deviates More

39
Kinetic Theory
  • Summary
  • pressure is a measure of the total kinetic energy
    of molecules, the force per unit area of these
    molecules
  • temperature is proportional to the average
    kinetic energy of molecules
  • from this kinetic theory viewpoint, we can derive
    the perfect gas law

40
Kinetic Theory
  • We will return to the perfect gas law from a
    macroscopic point of view and derive exactly the
    same relationship

where ... p pressure V volume, n number of
moles N number of molecules T temperature k
Boltzmann constant m mass, M molecular weight
or
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