According to kinetic theory the gas molecules are in a state of constant rapid motion in all possible directions colloiding in a random manner with one another and with the walls of the container and between two successive collisions molecules travel in a straight line path but show haphazard motion due to collisions.
States of Matter: Gases and Liquids
Partial Pressure Ratio of Nitrogen to Oxygen : The partial pressure of a gas is calculated using its mole fraction.
The mole fraction is the ratio of the number of moles of the gas to the total number of moles of all gases.
For nitrogen (), the mole fraction can be simplified as .
For oxygen (), the mole fraction is .
Therefore, the ratio of the partial pressure of nitrogen to oxygen is :
Partial Pressure Ratio of Oxygen to Argon : For argon (), the mole fraction is .
The ratio of the partial pressure of oxygen to argon is :
Root mean square (rms) velocity of N2 molecule (u) =
. For N2 molecule, molecular mass, M = 28. Therefore,
.....
(1) When the temperature becomes doubled, that is, 2T.
Let the new root mean square (rms) velocity of N-atom be u'.
For N-atom, the molecular mass, M = 14.
Therefore,
....... (2) On dividing Eq. (1) by Eq. (2), we get
The value of
is a measure of the magnitude of the attractive forces between the molecules of the gas. Greater the value of
larger is the attractive inter-molecular force between the gas molecules. The value of
related to the effective size of the gas molecules. It is also termed as excluded volume. The gases with higher value of
and lower value of
are more liquefiable, hence for
should be greater than for
but for it
should be less than for
Let the mass of methane and oxygen
Mole fraction of
Partial pressure of
Total pressure mole fraction of
We know, PV = nRT Given, P = 200 Pa V = 10 m3 T = 1000 K n = 0.5 + x 200 10 = (0.5 + x) R 1000 0.5 + x =
x =
x =
According to van der Waals' equation, for one mole of a gas
...... (1) At high pressure,
can be neglected So,
...... (2) From Eqs. (1) and (2), we get
Dividing both the sides by RT, we get
Compressibility factor
(For one mole of real gas) van der Waals equation
At low pressure, volume is very large and hence correction term
can be neglected in comparison to very large volume of
i.e.
Hence,
Weight of empty glass vessel = 40 gm Weight of glass vessel filled with liquid = 135 gm Weight of liquid = 135 40 = 95 gm Given density of liquid = 0.95 gm ml1 Volume of liquid
ml Weight of glass filled with ideal gas = 40.5 gm Weight of gas = 40.5 40 = 0.5 g Let the Molar mass = M Moles of gas
Now applying ideal gas equation, pV = nRT
M = 0.5 250 = 125 g/mol
The van der Waals constant 'a' is a measure of the strength of the intermolecular forces in a gas.
Larger molecules and molecules with stronger intermolecular forces will have larger 'a' constants.
Here, we are comparing argon (Ar), methane (CH₄), water (H₂O), and benzene (C₆H₆).
Argon (Ar) is a noble gas and is monoatomic.
Methane (CH₄) is a small molecule with weak intermolecular forces.
Water (H₂O) is a small molecule but has strong hydrogen bonding, making its intermolecular forces stronger than those in methane.
Benzene (C₆H₆) is a larger molecule than the others and has relatively strong intermolecular forces due to its larger size and polarizability.
So, in the increasing order of van der Waals constant 'a', it should be: Argon (Ar) < Methane (CH₄) < Water (H₂O) < Benzene (C₆H₆)