2.1.2

Molecular Kinetic Theory Model 2

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Average molecular kinetic energy

The average molecular energy can be used to find the pressure of radiation.

Kinetic energy

Kinetic energy

  • We assume that a gas is homogeneous (the same everywhere) and isotropic (has the same value when measured in different directions).
  • This means that the average speed of a molecule in the x-direction must be the same as the y and the z-directions. So we can write:
    • vx=vy=vZ{v_x}={v_y}={v_Z}
  • This means that the average kinetic energy in each direction is the same.
Momentum

Momentum

  • We consider a cube of length l which contains a gas.
  • If we only look at the x-direction, we can say that the time taken for a particle to travel from one end to the other is:
    • t=lvxt=\frac{l}{{v_x}}
  • If a particle collides with the wall of the box and is absorbed, we can write the change in momentum as:
    • Change in momentum = mass x velocity
    • P=mvxP=m{v_x}
Force

Force

  • We can write the force exerted on the wall when it absorbs a particle as:
    • Force = change in momentum ÷ change in time
    • F=PtF=\frac{P}{t}
  • We can substitute in the equations for momentum and time to get:
    • F=mvx2lF=\frac{m{v_x}^2}{l}
Pressure

Pressure

  • The pressure on the wall of the box when it absorbs one particle is given by the equation:
    • Pressure = force ÷ area
    • p=FAp=\frac{F}{A}
  • We can use the value for force and that the area is length squared to get:
    • p=mvx2l3p=\frac{m{v_x}^2}{l^3}
  • Since volume is length cubed we get:
    • p=mvx2Vp=\frac{m{v_x}^2}{V}
Pressure 2

Pressure 2

  • We have found the pressure for one particle if N particles hit the wall the pressure would be:
    • Total pressure = number of particles x pressure from one particle.
    • pt=Np{p_t}=Np
  • We can substitute the pressure in to give:
    • pt=Nmvx2V{p_t}=N\frac{m{v_x}^2}{V}
Kinetic equation

Kinetic equation

  • Recalling that the velocity is the same in all directions, we can write an equation for the total velocity squared as:
    • vt2=vx2+vy2+vz2{v_t}^2= {v_x}^2+{v_y}^2+{v_z}^2
  • Because the velocities are equal, we can simplify to give:
    • vx2=13vt2{v_x}^2=\frac{1}{3}{v_t}^2
  • So the equation for pressure can be written as:
    • pV=13Nmv2pV=\frac{1}{3}Nmv^2

Molecular Kinetic Theory - Developments Over Time

Ideas about the underlying structure of materials have changed considerably over time.

Early ideas

Early ideas

  • The idea that the atom, or atoms that are too small to directly view, move around is ancient. This dates from Lucretius in approx 50 BCE.
  • This idea was largely ignored because of the predominance of Aristotelian ideas about elements such as fire, earth, air and water.
Particle nature of matter

Particle nature of matter

  • The modern theory of the particle nature of matter was attributed to Bernoulli.
  • This was prior to the ideas of conservation of energy and how collisions between particles could be elastic.
  • The model did not predict anything in itself.
More complex ideas

More complex ideas

  • Clausius developed a much more complex set of ideas.
  • The observation of Brownian motion is the first direct evidence of the existence of particles.
  • The kinetic theory of gases became universally accepted because of Einstein and Smoluchowski’s theoretical model, which made specific predictions about Brownian motion and diffusion.
Jump to other topics
1

Space, Time & Motion

2

The Particulate Nature of Matter

3

Wave Behaviour

4

Fields

4.1

Circular Motion

4.2

Newton's Law of Gravitation

4.3

Fields

4.4

Fields at Work

4.5

Electric Fields

4.6

Magnetic Effect of Electric Currents

4.7

Heating Effect of Currents

4.8

Electromagnetic Induction

4.9

Power Generation & Transmission

4.10

Capacitance

5

Nuclear & Quantum Physics

6

Measurements

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