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Showing posts with label molar heat capacity. Show all posts
Showing posts with label molar heat capacity. Show all posts

Wednesday, October 6, 2010

AP Physics B - Multiple Choice Practice Questions on Kinetic Theory of Gases

Essential points to be remembered in kinetic theory of gases were discussed in the post dated 13th March 2008. Questions on kinetic theory of gases were discussed subsequently. You can access all posts related to kinetic theory of gases by clicking on the label, ‘kinetic theory’ below this post. To access older posts you need to click on the ‘older posts’ button.

Today we will discuss a few more typical multiple choice questions on kinetic theory of gases:

(1) The root mean square (R.M.S.) speed v of the molecules of an ideal gas is given by the expressions,

v = √(3RT/M ) and

v = √(3kT/m ) where R is universal gas constant, T is the absolute (Kelvin) temperature, M is the molar mass, k is Boltzman’s constant and m is the molecular mass. The R.M.S. speed of oxygen molecules (O2) at temperature T1 is v1. When the temperature is doubled, if the oxygen molecules are dissociated into atomic oxygen, what will be R.M.S. speed of oxygen atoms? (Treat the gas as ideal).

(a) v1/2

(b) v1

(c) √2 v1

(d) 2v1

(e) 4v1

We have v1 = √(3RT1/M ) or

v1 = √(3kT1/m )

On dissociation the molar mass as well as the molecular mass gets halved. Using the second equation, the R.M.S. speed v after dissociation is given by

v = √[3k×2T1/ (m/2 )] = 2√(3kT1/m ) = 2v1

(2) Four moles of an ideal diatomic gas is heated at constant volume from 20º C to 30º C. The molar specific heat of the gas at constant pressure (Cp) is 30.3 Jmol–1K–1 and the universal gas constant (R) is 8.3 Jmol–1K–1. The increase in internal energy of the gas is

(a) 80.3 J

(b) 303 J

(c) 332 J

(d) 880 J

(e) 1212 J

The increase in internal energy is MCvT where M is the mass of the sample of the gas, Cv is the specific heat at constant volume and T is the rise in temperature of the gas. If we use the molar specific heat of the gas at constant volume for Cv, the number of moles in the sample of the gas is to be used in the place of M.

Now, Cv = Cp R = 30.3 – 8.3 = 22 Jmol–1K–1.

Therefore, the increase in internal energy of the gas is 4×22×10 = 880 J.

(3) In the case of real gases, the equation of state, PV = RT (where P, V and T are respectively the pressure, volume and absolute temperature), is strictly satisfied only if corrections are applied to the measured pressure P and the measured volume V. The corrections for P and V arise respectively due to

(a) intermolecular attraction and the size of molecules

(b) size of molecules and expansion of the container

(c) expansion of the container and intermolecular attraction

(d) kinetic energy of molecules and collision of molecules

(e) intermolecular attraction and collision of molecules

In kinetic theory of gases it is assumed that there is no force between molecules But there is actually intermolecular attraction which reduces the pressure. So the correction for P arises due to intermolecular attraction.

The entire volume V of the container is not available for the molecules since the molecules have a finite size. The assumption (in kinetic theory) that the molecules are point masses without appreciable volume is incorrect. So the correction for V arises due to the size of molecules.

The correct option is (a).

(4) Gases exert pressure on the walls of the container because the gas molecules

(a) collide one another

(b) exert intermolecular attraction

(c) possess momentum

(d) expand on absorbing heat

(e) exert repulsive force

Because of the momentum of the gas molecules, they collide with the walls of the containing vessel and momentum transfer takes place, resulting in a force on the walls. Pressure is force per unit area. The basic reason for the pressure is the momentum of the gas molecules [Option (c)].

Now, see similar questions with solution here.

Thursday, March 13, 2008

AP Physics B– Kinetic Theory of Gases – Equations to be Remembered

You will have to remember certain basic formulae for solving multiple choice questions within the permitted time. The essential things you need to remember in kinetic theory of gases are given below:

(1) Pressure exerted by a gas, P = (1/3) nmc2 = (1/3)ρc2 where ‘n’ is the number of molecules per unit volume, ‘m’ is the molecular mass, ‘c’ is the r.m.s. speed of the gas molecule and ρ’ is the density of the gas.

(2) A very useful expression for the pressure of a gas is P = nkT where ‘k’ is Boltzman’s constant and T is the absolute temperature (Kelvin scale).

(3) Root mean square (R.M.S.) speed of gas molecule, c = √(3P/ρ) = √(3kT/m).

This can be rewritten in terms of the molar mass M and the universal gas constant R as

c = √(3RT/M)

(4) Since translational motion along three directions only are possible in our three dimensional space, the average translational kinetic energy of any type of gas molecule is (3/2)kT

(5) If the molecule has ‘f’ degrees of freedom, the average kinetic energy per molecule is (f/2 )kT.

Note the following points in this context (bearing in mind that the energy per degree of freedom is ½ kT):

(i) A mono atomic gas molecule has 3 degrees of freedom and has translational kinetic energy only [equal to (3/2)kT ].

(ii) A diatomic gas molecule has 5 degrees of freedom (three translational and two rotational) and hence the total average kinetic energy per molecule is (5/2 )kT.

(iii) Tri-atomic and polyatomic gas molecules have 6 degrees of freedom (three translational and three rotational). The total average kinetic energy per molecule is ( 6/2 )kT = 3kT.

(6) The kinetic energy. per mole in all the above cases is N times the kinetic energy of a molecule where N is the Avogadro number. Since Nk=R, the average K.E. per mole is (3/2 )RT for mono atomic, (5/2 )RT for diatomic and 3RT for triatomic and polyatomic gas molecules.

(7) The molar heat capacity (molar specific heat) at constant volume (CV) is obtained by putting T = 1 (corresponding to a temperature rise of 1K) in the above expressions. The values are therefore (3/2 )R for mono atomic gas, (5/2 )R for diatomic gas and 3R for tri atomic and polyatomic gases.

(8) The molar heat capacity (molar specific heat) of a gas at constant pressure (CP) is given by

CP = CV + R. This is Meyer’s relation.

Therefore, the values of CP are (5/2)R for mono atomic gas, (7/2)R for diatomic gas and 4R for tri and poly atomic gases.

(9) The ratio of specific heats of a gas is γ = CP/CV

The ratio of specific heats ‘γ’ is related to the number of degrees of freedom ‘f’' as

γ = 1+ (2/f)

[You should note that in the above discussion, the vibrational modes of the molecules have not been considered. Even though the above values are in agreement with the values obtained from experiment in the case of several gases, there are discrepancies in the case of certain diatomic gases and several polyatomic gases. In a more rigorous treatment, the vibrational modes also are to be taken into account; but the above discussion is sufficient at the moment].

In the next post, questions on kinetic theory will be discussed. Meanwhile, find some useful posts in this section here