Physic 11th Kinetic Theory Of Gases

Kinetic Theory Of Gases

1. Gas Laws

Gas laws are study of any two of quantities like pressure, volume and temperature, when the third is kept constant

A. Boyle's law


• "At constant temperature, the volume of a given mass of gas is invesely propertional to pressure." Thus
                 V ∝ 1/P
  Or,                PV = constant               (1)
• If P₁, V₁are initial pressure and volumes and P₂, V₂be final values then,            
       P₁V₁= P₂V₂                    
• Graph between P and V at temperature T₁ and T₂ such that T₁<T₂ are shown below,
  
   
• Graph above shows that Boyle's law is strictly not obeyed by gases at all values of P and T but it obeys this law only at low pressure and high temperature i.e., at law density

B. Charle's Law 

• Charle's Law is stated as follows :
  "When pressure of a gas is constant the volume of a given mass of gas is directly proportional to its absolute temperature".
                 V/T = Constant               (2)
• Graph between V and T is
  
  
  This graph shows that experimental graph deviates from straight line. Theoritical and enperimental graphs are in agreement at high temperature.

2. Ideal gas equation

• We can combine Boyle’s law eqn (1) and charle’s law eqn (2) in to a single eqn i.e.,
       PV/T = Constant          (3)
  If n moles is the mass of gas then we write
       PV = nRT               (4)
  where, n is number of moles of gas, R=N_AK_B is the universal constant known as gas constant and T is the absolute temperature.
• A gas satisfying eqn (4) at all values of presserves and temperatures is said to be an ideal gas
  now no of moles of gas
       n = m/M = N/N_A
  where
       m - mass of gas containing N molecules
       M - molar mass
       N_A - Avagadro’s number.
  From this,
       P = ρRT/M
       ρ - mass density of gas.

3. Moleular nature of matter

• We know that molecules which are made up of one or more atoms constitute matter.
• In solids these atoms and molecules are rigidly fixed and space between then is very less of the order of few angestrem and hance they can not move.
• In liquids these atoms and molecules can more enabeling liquids to flow.
• In gases atoms are free to travell without colliding for large distances such that if gases were not enclosed in an enclosure they would disappear.

4. Dalton's law of partial pressures :

• Consider a mixture of non-interacting ideal gases with n₁ moles of gas 1,n₂ of gas 2 and so on
• Gases are enclosed in an encloser with volume V, temperature T and pressure P.
• Equation of state of mixture
       PV = (n₁+ n₂)RT
  or     P = n₁RT/V + n₂RT/V + - - - -
        = P₁ + P₂ + - - --
  where,
       P₁ = n₁RT/V
  is pressure the gas 1 would exert at same V and T if no other gases were present in the enclosure. This is know as law of partial pressure of the gases.
• The total pressure of mixture of ideal gases is sum of partial pressures of individual gases of which mixture is made of.

5. Kinetic Theory of an ideal gas

Following are the fundamental assumptions of kinetic theory of gases.

• Gas is composed of large number of tiny invisible particles know as molecules
• These molecules are always in state of motion with varying velocities in all possible directions.
• Molecules traverse straight line path between any two collisions
• Size of molecule is infinitely small compared to the average distance traverse by the molecules between any two consecutive collisions.
• The time of collision is negligible as compared with the time taken to traverse the path.
• Molecules exert force on each other except when they collide and all of their molecular energy is kinetic. 
• Intermolecular distance in gas is much larger than that of solids and liquids and the molecules of gas are free to move in entire space free to them.

6. Pressure of gas

• Consider a cubical vessel with perfectly elastic walls containing large number of molecules say N let l be the dimension of each side of the cubical vessel.
• v_1x , v_1y, v_1z be the x, y, and z componenet of a molecule with velocity v.
• Consider the motion of molecule in the direction perpandicular to the face of cubical vessel.
• Molecule strikes the face A with a velocity v_1x and rebounds with the same velocity in the backward direction as the collisions are perfectly elastic.
  
   
• If m is the mass of molecule, the change in momentum during collision is
       mv_1x - (-mv_1x) = 2 mv_1x          (1)
• The distance travelled parallel to x-axis an is between A to A´ and when molecule rebounds from A´and travel towards A is 2L
• Time taken by molecule to go to face A´ and then comeback to A is
            Δt = 2l/v_1x
• Number of impacts of this molecule with A in unit time is
       n = I/Δt = v_1x/ 2l               (2)
  Rate of change of momentum is
       ΔF = ΔP/Δt
       =nΔP
  from (1) and (2)
       ΔF = mv_1x² / l
  this is the force exerted on wall A due to this movecule.
• Force on wall A due to all other molecules
       F = Σmv_1x²/L           (3)
• As all directions are equivalent
  Σv_1x²=Σv_1y²=Σv_1z²
  Σv_1x²= 1/3Σ((v_1x)² + (v_1y)² +( v_1z)² )
       = 1/3 Σv₁²
  Thus     F = (m/3L) Σv₁²
• N is total no. of molecules in the container so
       F = (mN/3L) (Σ(v₁)²/N)
• Pressure is force per unit area so
       P = F/L²
        =(M/3L³)(Σ(v₁)²/N)
  where ,M is the total mass of the gas and if ρ is the density of gas then
       P=ρΣ(v₁)²/3N
  since Σ(v₁)²/N is the average of squared speeds and is written as v_mq² known as mean square speed
  Thus, v_rms=√(Σ(v₁)²/N) is known as roon mean squared speed rms-speed and v_mq² = (v_rms)²
• Pressure thus becomes
       P = (1/3)ρv_mq²                     (4)
  or     PV = (1/3) Nmv_mq²                     (5)
  from equation (4) rms speed is given as
       v_rms = √(3P/ρ)
                 = √(3PV/M)                    (6)

7. Kinetic interpretation of temperature

• From equation (5) we have
       PV = (1/3)Nmv_mq²
  where N is the number of molecules in the sample. Above equation can also be written as
       PV = (2/3)N(1/2)Nmv_mq²                (7)
• The quantity (1/2)Nmv_mq² in equation (7) is the kinetic energy of molecules in the gas. Since the internal energy of an ideal gas is purely kinetic we have,
       E=(1/2)Nmv_mq²                     (8)
• Combining equation 7 and 8 we get
       PV=(2/3)E
• Comparing this result with the ideal gas equation (equation (4) ) we get
       E=(3/2)K_BNT
  or,     E/N=(1/2)mv_mq² =(3/2)K_BT          (9)
  Where, K_B is known as Boltzmann constant and its value is K_B=1.38 X 10^-23 J/K
• From equation (11) we conclude that the average kinetic energy of a gas molecule is directly proportional to the absolute temperature of the gas and is independent of the pressure , volume and nature of the gas.
• Hence average KE per molecule is
       (1/2)mv²¯=(3/2)K_BT
  from this since v²¯=(v_rms)², rms velocity of a molecule is
       v_rms=√(3K_BT/m)                    (10)
  This can also be written as
       v_rms=√(3K_BNT/Nm)
        =√(3RT/M)                    (11)
  where, M=mN is the molecular mass of the gas.
  
  Assignment
  (1)Gas laws (Boyle's and charle's law) and perfect gas equation can be derived using kinetic theory of gases. try to derive them.

7. Law of Equipartition of energy

• According to the principle of equipartition of energy, each velocity component has, on the average, an associated kinetic energy (1/2)KT.
• The number of velocity components needs to describe the motion of a molecule completely is called the number of degrees of freedom.
• For a mono atomic gas there are three degrees of freedom and the average total KE per molecule for any monotomic gas is 3/2 K_BT.
       

8. Specific Heat Capacity

(i) Monoatomic gases :

• Monoatemic gas moleules has three translational degrees of freedom.
• From law of equipartition of energy average energy of an molecule at temperature T is (3/2)K_BT
• Total internal energy of one mole of such gas is
       U= (3/2)K_BTN
        = (3/2) RT                    (12)
• If C_V is melar specific heat at constant volume then
       C_Vv = dU/dT
        = (3/2)R                         (13)
  now for an ideal gas
       C_P - C_V = R
  C_P - molar specific heat capacity at constant presseve
       C_P = 5/2 R                    (14)
  Thus for a monoatomic gas ratio of specific heats is
       γ_mono = C_P/C_V= 5/3               (15)

(ii) Diatomic gases :

• A diatomic gas molecule is treated as a rigid rotator like dumb-bell and has 5 degrees of freedom out of which three degrees of freedom are translatoinal and two degrees of freedom are rotational.
• Using law of equipartition of energy the total internal energy of one mole of diatomic gas is
       U= (5/2)K_BTN
       = (5/2) RT                    (16)
• Specific heats are thus
       C_V =(5/2)R
       γ_dia= 5/7          (rigid rotater)
• If diatomic molecule is not only rigid but also has an vibrational mode in addition, then
       U = (7/2) RT
       and C_V=(7/2)R
       C_P=(9/2)R
  and γ=C_P/C_V=9/7

9. Specific heat Capacity of Solids

• From law of equipartation of energy we can can also determine specific heats of solids.
• Consider that atoms in a solid are vibrating about their mean position at some temperature T.
• Oscillation in one dimension has average energy equals 2(1/2)K_BT=K_BT, as (1/2)K_BT is PE and (1/2)K_BT is KE of the atom.
• In three dimensions average kinetic energy is 3K_BT.
• For one mole of solid total energy is
       U= 3NK_BT
        = 3RT
• At constant pressure ΔQ =ΔU+PΔV=ΔU since for solids ΔV is negligible hence
       C=ΔQ/ΔT=ΔU/ΔT=3R
• This is Dulang and Petit law.
• Here we note that predictions of specific heats of solids on the basis of law of equipetation of energy are independent of temperature.
• As we go towards low temperatures T→0 there is a pronounced departure from the value of specific heat of solids as calculated.
• It is seen that specific heats of substance aproaches to zero as T→0.
• This result can further be explained using the principles of quantum mechanics which is beyond our scope.

10. Mean free Path

• On the basis of kinetic theory of gases, it is assumed that the molecules of a gas are continously collilding against each other.
• Molecules move in straight line with constant speeds between two successive collisions.
• Thus path of a single molecule is a series of zig-zag paths of different lengths as shown in fig -.
  
   
• These paths of different lengths are called free paths of the molecule
• Mean Free Path is the averege distance traversed by molecule between two successive collisions.
• If s is the Total path travelled in N_coll coilisions, then mean free path
       λ= s/N_coll
  Expression for mean free path :
• Consider a gas containing n molecules per unit volume.
• We assume that only one molecule which is under consideration is in motion while all others are at rest.
• If σ is the diameter of each molecule then the moving molecule will collide with all these molecules where centers lie within a distance from its centre as shown in fig
  
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• If v is the velocity of the moving molecule then in one second it will collide with all moleculeswith in a distance σ between the centres.
• In one second it sweeps a volume πσ²v where any other molecule will collide with it.
• If n is the total number of molecules per unit volume, then nπσ²v is number of collisions a molecule suffers in one second.
• If v is the distance traversed by molecule in one second then mean free path is given by
       λ = total distance traversed in one second /no. of collision suffered by the molecules
        =v/πσ²vn
        =1/πσ²n
• This expression was derived with the assumption that all the molecules are at rest except the one which is colliding with the others.
• However this assumption does not represent actual state of affiar.
• More exact statement can be derived considering that all molecules are moving with all possible velocities in all possible directions.
• More exact relation found using distribution law of molecular speeds is
       λ=1/(√2)πσ²n
  its derivation is beyond our scope.

Solved examples

Question-1.Let A & B are two sample of ideal gases of equal mole .let T be the temperature of both the gas Let E_A and E_Bare there total energy respectively .Let M_A and M_B are these respective molecular mass .which of these is true
a,E_A > E_B
b,E_A < E_B
c,E_A =E_B
d,none of these

Solution:1
E_A = 3/2 nRT
E_B = 3/2 nRT
;E_A =E_B


Question-2. The velocities of the molecules are v, 2v, 3v, 4v & 5v. The rms speed will be
a,11v
b,v(11)^1/2
c, v
d, 3.3v

Solution:2
Vrms= (∑ V² / N)^1/2
= [(V² + 4V² + 9V² + 16V² + 25V²)/5]^1/2
=v(11)^1/2

Question-3:
An ideal gas A is there.Intial temperature is 27°C.The temperature of the gas is increased to 927°C.Find the ratio of final V_rmsto the initial V_rms 

Solution-9:

V_rms=√3RT/M

So it is proportional to Temperature
Now 
T₁=27°C =300K
T₂=927°C =1200K

So intial V_rms=k√300
Final V_rms=k√1200

ratio of final to intial=2:1


Question-.4 Two absolute scales A and B have triple points of water defined as 200A and 350A. what is the relation between T_A and T_B



Solution-4

Given that on absolute scale
Triple point of water on scale A = 200 A
Triple point of water on scale B = 350 B
Also, triple point of water on Kelvin scale = 273.16 K
Now temperature on scale A and on scale B is equivalent to 273.16 K on absolute temperature scale.
Thus, value of one degree on absolute scale A = (273.16/200) K
Or, 
Value of temperature T_A on absolute scale A = (273.16XT_A)/200 
Similarly value of temperature T_B on absolute scale B = (273.16XT_B)/350
Since T_A and T_B represent the same temperature
273.16×T_A/200 = 273.16×T_B/350
Or, T_A = 200T_B/350 = 4T_B/ 7 

Question-.5 . which one is not the assumption in kinetic theory of gases
a.the molecules of the gas are in continual random motion
b. The molecules interact during the collison
c. The molecules are tiny hard sphere undergoing inelastic collision
d. The collison are of short duration
Solution-5

Answer is c

Question-.6. 
There are two statement
A. Equal volumes of all gases at the same temperature T and pressure P contain an equal no of Molecules
B.the no of molecules in one mole of any gas is 6.0255 * 10²².
which one of the following is correct
a. A and B both
b. A only 
c B only
d. A and B both are incorrect
Solution-6
Answer is b

Question-.7. .There are two statement about Ideal gases
A. The V_rms of gas molecules depends on the mass of the gas molecule and the temperature
B. The V_rms is same for all the gases at the same temperature
which one of the following is correct
a. A and B both
b. A only 
c B only
d. A and B both are incorrect
Solution-7

Answer is b

Question-.8. .Choose the correct statement of the following
a. The pressure of the gas is equal to the total kinetic energy of the molecules in a unit volume of the gas
b. The product of pressure and volume of the gas is always constant
c. The average kinetic energy of molecule of the gas is proportional to its absolute temperature
d. The average kinetic energy of molecule of the gas is proportional to the square root of its absolute temperature
Solution-8

Answer is c

Question-.9...which one is true according Vander Waal gas equation
a. The attractive forces between the molecules is not negligible
b Volume of the molecules is negligible as compared to the volume occupied by the gas
c. Volume of the molecules is not negligible as compared to the volume occupied by the gas
d. The attractive forces between the molecules is negligible
Solution-9
Answer is a,c