Mean free path
- Mean free path is the average distance between the two successive collisions.
- Inside the gas there are several molecules which are randomly moving and colliding with each other.
- The distance which a particular gas molecule travels without colliding is known as mean free path.
Expression for mean free path
- Consider each molecule of gas is a sphere of diameter (d).The average speed of each molecule is<v>.
- Suppose the molecule suffers collision with any other molecule within the distance (d). Any molecule which comes within the distance range of its diameter this molecule will have collision with that molecule.
- The volume within which a molecule suffer collision =<v>Δtπd2.
- Let number of molecules per unit volume =n
- Therefore the total number of collisions in time Δt =<v>Δtπd2xn
- Rate of collision =<v>Δtπd2xn/Δt=<v>πd2n
- Suppose time between collision τ =1/<v>πd2n
- Average distance between collision = τ<v> = 1/πd2
- 1/πd2n this value was modified and a factor was introduced.
- Mean free path(l) = 1/√2 π d2n
Conclusion: – Mean free path depends inversely on:
- Number density (number of molecules per unit volume)
- Size of the molecule.
Temperature inside the cylinder, T = 17°C =290 K
Radius of a nitrogen molecule, r = 1.0 Å = 1 × 1010 m
Diameter, d = 2 × 1 × 1010 = 2 × 1010 m
Molecular mass of nitrogen, M = 28.0 g = 28 × 10–3 kg
The root mean square speed of nitrogen is given by the relation:
R is the universal gas constant = 8.314 J mole–1 K–1
Therefore vrms=√ (3×8.314×290)/ (28×10-3)
The mean free path (l) is given by the relation:
Where, k is the Boltzmann constant = 1.38 × 10–23 kgm2 s–2K–1
Therefore l= 1.38×10-23x290/√2x 3.14x (2×10-10)2x2.026×105
= 1.11 × 10–7 m
= 4.58 × 109 s–1
Collision time is given as:
= 2×10-10/508.26 = 3.93 × 10–13 s
Time taken between successive collisions:
T’=l/vrms = 1.11×10-7m/508.26m/s= 2.18 × 10–10 s
T’/T= 2.18 × 10–10 s/3.93×10-13 = 500
Hence, the time taken between successive collisions is 500 times the time taken for a collision.