Advertisements
Advertisements
प्रश्न
Estimate the mean free path and collision frequency of a nitrogen molecule in a cylinder containing nitrogen at 2.0 atm and temperature 17 °C. Take the radius of a nitrogen molecule to be roughly 1.0 Å. Compare the collision time with the time the molecule moves freely between two successive collisions (Molecular mass of N2 = 28.0 u).
उत्तर १
Mean free path = 1.11 × 10–7 m
Collision frequency = 4.58 × 109 s–1
Successive collision time ≈ 500 × (Collision time)
Pressure inside the cylinder containing nitrogen, P = 2.0 atm = 2.026 × 105 Pa
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:
`v_"rms" = sqrt((3RT)/M)`
Where
R is the universal gas constant = 8.314 J mole–1 K–1
`:. v_"rms" = sqrt((3xx8.314xx290)/(28xx10^(-3))) = 508.26 "m/s"`
The mean free path (l) is given by the relation:
`l = kT/(sqrt2xx d^2xx P)`
Where,
k is the Boltzmann constant = 1.38 × 10–23 kg m2 s–2K–1
`:. l = (1.38xx10^(-23)xx290)/(sqrt2 xx 3.14 xx (2xx10^(-10))^2 xx 2.026 xx 10^5)`
`= 1.11 xx 10^(-7) m`
Collision frequency = `v_"rms"/l`
`=508.26/(1.11xx10^(-7)) = 4.58 xx 10^(9) s^(-1)`
Collision time is given as:
`T = d/v_"rms"`
`= (2xx10)^(-10)/508.26 = 3.93 xx 10^(-13) s`
Time taken between successive collisions:
`T' = 1/v_"rms"`
`= (1.11 xx 10^(-7))/(508.26 "m/s") = 2.18 xx 10^(-10) s`
`:. "T'"/T = (2.18xx 10^(-10))/(3.93xx10^(-13)) = 500`
Hence, the time taken between successive collisions is 500 times the time taken for a collision.
उत्तर २
Here `P = 2.0 " atm" = 2 xx 1.013 xx 10^5 Pa = 2.026 xx 10^5 Pa`
`T = 17 ^@C = 17 + 273 = 290`
Radius `R = 1.0 Å = 1 xx 10^(-10) m` = Molecular mass = 28 u
`:. m = 28 xx 1.66 xx 10^(-27) = 4.65 xx 10^(-26) kg`
Also R = 8.31 `J mol^(-1) K^(-1)`, `k = 1.38 xx 10^(-23) JK^(-1)`
Now for one mole of a gas, `PV = RT => V = RT/P = (8.31 xx 290)/(2.026 xx 10^5)`
`=> V = 1.189 xx 10^(-2) m^3`
:. Number of molecules per unit volume , ` n = N/V`
`:. n = (6.023 xx 10^(23))/(1.189xx10^(-2)) = 5.06 xx 10^(25) m^(-3)`
Now, mean free path, `lambda = 1/(sqrt(2)pind^2) = 1/(sqrt(2)pin(2r)^2)`
`= 1/(1.414 xx 3.14xx 5.06xx 10^25xx (2xx1xx10^(-10))^2`
`= 1.1 xx 10^(-7)`
Also `v_"rms" = sqrt((3RT)/M) = sqrt((3xx8.31xx290)/(28xx10^(-3))) = 5.08 xx 10^2 ms^(-1)`
:. Collision frequency, `v = v_"rms"/lambda = (5.08 xx 10^2)/(1.1 xx 10^(-7)) = 4.62 xx 10^9 s^(-1)`
Time between successive collisions =` 1/v = 1/(4.62 xx 10^9) = 2.17 xx 10^(-10)s`
Also the collision time = `d/v_"rms" = (2xx1xx10^(-10))/(5.08 xx 10^2)s = 3.92 xx 10^(-13) s`
APPEARS IN
संबंधित प्रश्न
Choose the correct option.
The mean free path λ of molecules is given by where n is the number of molecules per unit volume and d is the diameter of the molecules.
If the temperature and pressure of a gas is doubled the mean free path of the gas molecules ____________.
Define mean free path and write down its expression.
List the factors affecting the mean free path.
Derive the expression for the mean free path of the gas.
Calculate the mean free path of air molecules at STP. The diameter of N2 and O2 is about 3 × 10−10 m
Consider an ideal gas at pressure P, volume V and temperature T. The mean free path for molecules of the gas is L. If the radius of gas molecules, as well as pressure, volume and temperature of the gas are doubled, then the mean free path will be:
Mean free path of molecules of a gas is inversely proportional to ______.
Calculate the ratio of the mean free paths of the molecules of two gases having molecular diameters 1 A and 2 A. The gases may be considered under identical conditions of temperature, pressure and volume.
Ten small planes are flying at a speed of 150 km/h in total darkness in an air space that is 20 × 20 × 1.5 km3 in volume. You are in one of the planes, flying at random within this space with no way of knowing where the other planes are. On the average about how long a time will elapse between near collision with your plane. Assume for this rough computation that a saftey region around the plane can be approximated by a sphere of radius 10 m.