SlideShare a Scribd company logo
1 of 14
Download to read offline
1
CLASS XII
PHYSICS
CHAPTER 3
KINETIC THEORY OF GASES
AND RADIATION
Exercises
2
Kinetic Theory of Gases and Radiation
1. Choose the correct option:
i) In an ideal gas, the molecules possess
(A) only kinetic energy
(B) both kinetic energy and potential energy
(C) only potential energy
(D) neither kinetic energy nor potential energy
ii) The mean free path Ξ» of molecules is given by
where n is the number of molecules per unit volume and d is the diameter of
the molecules.
(A) √
2
πœ‹ 𝑛 𝑑2
(B)
1
πœ‹ 𝑛 𝑑2
(C)
1
√2 πœ‹ 𝑛 𝑑2
(D)
1
√2 πœ‹ 𝑛 𝑑
iii) If the pressure of an ideal gas decreases by 10% isothermally, then its volume
will _______.
(A) decrease by 9%
(B) increase by 9%
(C) decrease by 10%
(D) increase by 11.11%
iv) If a = 0.72 and r = 0.24, then the value of π‘‘π‘Ÿ is
(A) 0.02 (B) 0.04
(C) 0.4 (D) 0.2
v) The ratio of emissive power of perfect blackbody at 1327Β°C and 527Β°C is
(A) 4:1 (B) 16:1
(C) 2:1 (D) 8:1
2. Answer in brief:
i) What will happen to the mean square speed of the molecules of a gas if the
temperature of the gas increases?
Ans: If the temperature of a gas increases, the mean square speed of the
molecules of the gas will increase in the same proportion.
ii) On what factors do the degrees of freedom depend?
Ans: The degrees of freedom depend upon
(i) the number of atoms forming a molecule
(ii) the structure of the molecule
(iii) the temperature of the gas.
iii) Write ideal gas equation for a mass of 7 g of nitrogen gas.
Ans:
3
iv) If the density of oxygen is 1.44 kg/π‘š3
at a pressure of 105
N/π‘š2
, find the
root mean square velocity of oxygen molecules.
Ans:
v) Define athermanous substances and diathermanous substances.
Ans: Athermanous substances
Substances that don't allow transmission of infrared radiation through them
are called athermanous substances.
- For example, wood, metal, 𝐢𝑂2, water vapours, etc.
Diathermanous substances
Substances that allow transmission of infrared radiation through them are
called diathermanous substances.
- For example, rock salt, pure air, glass, etc.
3. When a gas is heated, its temperature increases. Explain this phenomenon on
the basis of the kinetic theory of gases.
Ans: Molecules of a gas are in a state of continuous random motion. They possess
kinetic energy. When a gas is heated, there is an increase in the average
kinetic energy per molecule of the gas. Hence, its temperature increases (the
average kinetic energy per molecule being proportional to the absolute
temperature of the gas).
4. Explain, on the basis of the kinetic theory of gases, how the pressure of a gas
changes if its volume is reduced at a constant temperature.
Ans: The average kinetic energy per molecule of a gas is constant at a constant
temperature. When the volume of a gas is reduced at a constant
temperature, the number of collisions of gas molecules per unit time with the
walls of the container increases. This increases the momentum transferred
per unit time per unit area, i.e., the force exerted by the gas on the walls.
Hence, the pressure of the gas increases.
4
5. Mention the conditions under which a real gas obeys ideal gas equation.
Ans: A real gas obeys the ideal gas equation when the temperature is very high
and pressure is very low [Note: Under these conditions, the density of a gas is
very low. Hence, the molecules, on average, are far away from each other.
The intermolecular forces are then not of much consequence.]
6. State the law of equipartition of energy and hence calculate the molar specific
heat of monatomic and diatomic gases at constant volume and constant
pressure.
Ans:
5
7. What is a perfect blackbody? How can it be realized in practice?
Ans: A perfect blackbody or simply a blackbody is defined as a body which absorbs
all the radiant energy incident on it. Fery designed a spherical blackbody which
consists of a hollow double-walled, metallic sphere provided with a tiny hole or
aperture on one side, Fig. The inside wall of the sphere is blackened with
lampblack while the outside is silver-plated. The space between the two walls is
evacuated to minimize heat loss by conduction and convection. Any radiation
entering the sphere through the aperture suffers multiple reflections where
about 97% of it is absorbed in each incidence by the coating of lampblack. The
radiation is almost completely absorbed after a number of internal reflections. A
conical projection on the inside wall opposite the hole minimizes the probability
of incident radiation escaping out.
When the sphere is placed in a bath of suitable fused salts, so as to maintain it at
the desired temperature, the hole serves as a source of black-body radiation. The
intensity and the nature of the radiation depend only on the temperature of the
walls.
6
A blackbody, by definition, has a coefficient of absorption equal to 1. Hence, its
coefficient of reflection and coefficient of transmission are both zero. The
radiation from a blackbody, called blackbody radiation, covers the entire range of
the electromagnetic spectrum. Hence, a blackbody is called a full radiator.
8. State
(i) Stefan-Boltzmann law.
Ans:
(ii) Wien's displacement law
Ans:
9. Explain the spectral distribution of blackbody radiation.
Ans:
i. The rate of emission per unit area or power per unit area of a surface is
defined as a function of the wavelength Ξ» of the emitted radiation.
ii. Scientists studied the energy distribution of blackbody radiation as a function
of wavelength.
iii. By keeping the source of radiation (such as a cavity radiator) at different
temperatures they measured the radiant power corresponding to different
wavelengths. The measurements were represented graphically in the form of
curves showing the variation of radiant power per unit area as a function of
wavelength Ξ» at different constant temperatures as shown in the figure.
10. Prove Kirchhoff’s law of radiation theoretically.
7
Ans: Consider an ordinary body O and perfectly black body B of the same
dimension suspended in a uniform temperature enclosure as shown in the figure.
At thermal equilibrium, both the bodies will have the same temperature as that
of the enclosure.
Let, E = emissive power of ordinary body O
Eb = emissive power of perfectly black body B
a = coefficient of absorption of O
e = emissivity of O
Q = radiant energy incident per unit time per unit area on each body.
Quantity of heat absorbed per unit area per unit time by body O = aQ.
Quantity of heat energy emitted per unit area per unit time by body O = E.
Since there is no change in temperature
E = aQ
Q = E/a .…(1)
Quantity of heat absorbed per unit area per unit time by a perfectly black body, B =
Q The radiant heat energy emitted per unit time per unit area by a perfectly black
body,
B = Eb
Since there is no change in temperature.
Eb = Q .…(2)
From equations (1) and (2),
11. Calculate the ratio of the mean square speeds of molecules of a gas at 30 K and
120 K.
Ans:
8
12. Two vessels A and B are filled with the same gas where the volume, temperature,
and pressure in vessel A is twice the volume, temperature, and pressure in vessel
B. Calculate the ratio of the number of molecules of the gas in vessel A to that in
vessel B.
Ans:
13. A gas in a cylinder is at pressure P. If the masses of all the molecules are made
one-third of their original value and their speeds are doubled, then find the
resultant pressure.
Ans:
14. Show that rms velocity of an oxygen molecule is √2 times that of a sulfur dioxide
molecule at S.T.P.
Ans:
9
15. At what temperature will oxygen molecules have same rms speed as helium
molecules at S.T.P.? (Molecular masses of oxygen and helium are 32 and 4
respectively).
Ans:
16. Compare the rms speed of hydrogen molecules at 127℃ with rms speed of
oxygen molecules at 27℃ given that molecular masses of hydrogen and oxygen
are 2 and 32 respectively.
Ans:
10
17. Find the kinetic energy of 5 litre of a gas at STP given the standard pressure is
1.013 Γ— 105
N/π‘š2
.
Ans:
18. Calculate the average molecular kinetic energy (i) per kmol (ii) per kg (iii) per
molecule of oxygen at 127Β°C, given that the molecular weight of oxygen is 32, R
is 8.31 J π‘šπ‘œπ‘™βˆ’1
πΎβˆ’1
and Avogadro’s number 𝑁𝐴 is 6.02 Γ— 1023
molecules π‘šπ‘œπ‘™βˆ’1
.
Ans:
11
19. Calculate the energy radiated in one minute by a blackbody of surface area 100
π‘π‘š2
when it is maintained at 227Β°C.
Ans:
20. Energy is emitted from a hole in an electric furnace at the rate of 20 W, when the
temperature of the furnace is 727Β°C. What is the area of the hole? (Take Stefan’s
constant Οƒ to be 5.7 Γ— 10βˆ’8
𝐽 π‘ βˆ’1
π‘šβˆ’2
πΎβˆ’4
)
Ans:
12
21. The emissive power of a sphere of area 0.02 π‘š2
is 0.5 kcal π‘ βˆ’1
π‘šβˆ’2
. What is the
amount of heat radiated by the spherical surface in 20 seconds?
Ans:
22. Compare the rates of emission of heat by a blackbody maintained at 727Β°C and
at 227Β°C, if the black bodies are surrounded by an enclosure (black) at 27Β°C.
What would be the ratio of their rates of loss of heat?
Ans:
13
23. The earth’s mean temperature can be assumed to be 280 K. How will the curve
of blackbody radiation look like for this temperature? Find out πœ†π‘šπ‘Žπ‘₯. In which
part of the electromagnetic spectrum, does this value lie?
Ans:
24. A small blackened solid copper sphere of radius 2.5 cm is placed in an evacuated
chamber. The temperature of the chamber is maintained at 100 Β°C. At what rate
must energy be supplied to the copper sphere to maintain its temperature at 110
Β°C? (Take Stefan’s constant Οƒ to be 5.67 Γ— 10βˆ’8
𝐽 π‘ βˆ’1
π‘šβˆ’2
πΎβˆ’4
and treat the
sphere as a blackbody.)
Ans:
14
25. Find the temperature of a blackbody if its spectrum has a peak at (a) πœ†π‘šπ‘Žπ‘₯ = 700
nm (visible), (b) πœ†π‘šπ‘Žπ‘₯= 3 cm (microwave region) (c) Ξ»max = 3 cm (FM radio
waves). (Take Wien’s constant b = 2.897 Γ— 10βˆ’3
m K).
Ans:

More Related Content

What's hot

Lecture9 1
Lecture9 1Lecture9 1
Lecture9 1guest2ac6ed
Β 
Implantation srim trim
Implantation  srim trimImplantation  srim trim
Implantation srim trimKamalakkannan K
Β 
The kinetic theory of gases
The kinetic theory of gasesThe kinetic theory of gases
The kinetic theory of gasesAshwani Kumar
Β 
Edexcel AS Physics Waves
Edexcel AS Physics WavesEdexcel AS Physics Waves
Edexcel AS Physics WavesPaul Burgess
Β 
Nuclear physics
Nuclear physicsNuclear physics
Nuclear physicsMustafa Gamal
Β 
Crystalography
CrystalographyCrystalography
Crystalographymd5358dm
Β 
Chapter 16 semiconductor devices
Chapter 16   semiconductor devices Chapter 16   semiconductor devices
Chapter 16 semiconductor devices Pooja M
Β 
Chapter 5 spectral lines of hydrogen atom
Chapter 5  spectral lines of hydrogen atomChapter 5  spectral lines of hydrogen atom
Chapter 5 spectral lines of hydrogen atomMiza Kamaruzzaman
Β 
Electrical polarization mechanisms
Electrical polarization mechanismsElectrical polarization mechanisms
Electrical polarization mechanismsDigvijaysinh Gohil
Β 
epitaxy deposition.ppt
epitaxy deposition.pptepitaxy deposition.ppt
epitaxy deposition.pptrahul177578
Β 
Mass defect and binding energy
Mass defect and binding energyMass defect and binding energy
Mass defect and binding energyLeilani Marcelo
Β 
Dielectrics and its applications
Dielectrics and its applicationsDielectrics and its applications
Dielectrics and its applicationsMohammed Limdiwala
Β 
Phonons lecture
Phonons lecturePhonons lecture
Phonons lectureOlbira Dufera
Β 
Epitaxy growth
Epitaxy growthEpitaxy growth
Epitaxy growthRutuja Solkar
Β 
X-ray diffraction technique (xrd)
X-ray diffraction technique  (xrd)X-ray diffraction technique  (xrd)
X-ray diffraction technique (xrd)saqib16
Β 
UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...
UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...
UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...University of California, San Diego
Β 
Elementary particles
Elementary particlesElementary particles
Elementary particlesSNS
Β 

What's hot (20)

Lecture9 1
Lecture9 1Lecture9 1
Lecture9 1
Β 
Photo electric effect and compton
Photo electric effect and comptonPhoto electric effect and compton
Photo electric effect and compton
Β 
Implantation srim trim
Implantation  srim trimImplantation  srim trim
Implantation srim trim
Β 
Chapter 6 x ray
Chapter 6 x rayChapter 6 x ray
Chapter 6 x ray
Β 
The kinetic theory of gases
The kinetic theory of gasesThe kinetic theory of gases
The kinetic theory of gases
Β 
Edexcel AS Physics Waves
Edexcel AS Physics WavesEdexcel AS Physics Waves
Edexcel AS Physics Waves
Β 
Nuclear physics
Nuclear physicsNuclear physics
Nuclear physics
Β 
Crystalography
CrystalographyCrystalography
Crystalography
Β 
Chapter 16 semiconductor devices
Chapter 16   semiconductor devices Chapter 16   semiconductor devices
Chapter 16 semiconductor devices
Β 
Chapter 5 spectral lines of hydrogen atom
Chapter 5  spectral lines of hydrogen atomChapter 5  spectral lines of hydrogen atom
Chapter 5 spectral lines of hydrogen atom
Β 
Electrical polarization mechanisms
Electrical polarization mechanismsElectrical polarization mechanisms
Electrical polarization mechanisms
Β 
epitaxy deposition.ppt
epitaxy deposition.pptepitaxy deposition.ppt
epitaxy deposition.ppt
Β 
Mass defect and binding energy
Mass defect and binding energyMass defect and binding energy
Mass defect and binding energy
Β 
Dielectrics and its applications
Dielectrics and its applicationsDielectrics and its applications
Dielectrics and its applications
Β 
Galilean Transformation Equations
Galilean Transformation EquationsGalilean Transformation Equations
Galilean Transformation Equations
Β 
Phonons lecture
Phonons lecturePhonons lecture
Phonons lecture
Β 
Epitaxy growth
Epitaxy growthEpitaxy growth
Epitaxy growth
Β 
X-ray diffraction technique (xrd)
X-ray diffraction technique  (xrd)X-ray diffraction technique  (xrd)
X-ray diffraction technique (xrd)
Β 
UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...
UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...
UCSD NANO106 - 03 - Lattice Directions and Planes, Reciprocal Lattice and Coo...
Β 
Elementary particles
Elementary particlesElementary particles
Elementary particles
Β 

Similar to Chapter 3 - Kinetic theory of gases and radiation exercises solution

revision xi - chapters1-5.pdf
revision xi - chapters1-5.pdfrevision xi - chapters1-5.pdf
revision xi - chapters1-5.pdfssuserfa137e1
Β 
Atomic structure presentation
Atomic structure presentationAtomic structure presentation
Atomic structure presentationNeeraj Yadav
Β 
Med.physics dr. ismail atomic and nuclear physics
Med.physics  dr. ismail atomic and nuclear physics Med.physics  dr. ismail atomic and nuclear physics
Med.physics dr. ismail atomic and nuclear physics Ismail Syed
Β 
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiationPHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiationPooja M
Β 
Quantum Mechanics Presentation
Quantum Mechanics PresentationQuantum Mechanics Presentation
Quantum Mechanics PresentationJasmine Wang
Β 
General Chemistry I - CHEM 181Critical Thinking Exercise.docx
General Chemistry I - CHEM 181Critical Thinking Exercise.docxGeneral Chemistry I - CHEM 181Critical Thinking Exercise.docx
General Chemistry I - CHEM 181Critical Thinking Exercise.docxbudbarber38650
Β 
Chapter-2-Prof-N.M.pptx
Chapter-2-Prof-N.M.pptxChapter-2-Prof-N.M.pptx
Chapter-2-Prof-N.M.pptxiqbalSIDDIQUEY
Β 
IIT JEE Physics 1995
IIT JEE Physics   1995IIT JEE Physics   1995
IIT JEE Physics 1995Vasista Vinuthan
Β 
Radiation lecture 1 nov 2013
Radiation lecture 1 nov 2013Radiation lecture 1 nov 2013
Radiation lecture 1 nov 2013apurbosu17
Β 
CBSE Class 11 Chemistry Sample ebook
CBSE Class 11 Chemistry Sample ebookCBSE Class 11 Chemistry Sample ebook
CBSE Class 11 Chemistry Sample ebookMiso Study
Β 
Stellar evolution 2015
Stellar evolution 2015Stellar evolution 2015
Stellar evolution 2015Paula Mills
Β 
Radiavtive Heat Transfer assignment
Radiavtive Heat Transfer assignmentRadiavtive Heat Transfer assignment
Radiavtive Heat Transfer assignmentAmritChatterjee3
Β 
Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)
Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)
Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)Dr. Sajid Ali Talpur
Β 

Similar to Chapter 3 - Kinetic theory of gases and radiation exercises solution (20)

revision xi - chapters1-5.pdf
revision xi - chapters1-5.pdfrevision xi - chapters1-5.pdf
revision xi - chapters1-5.pdf
Β 
Quantum theory of radiation
Quantum theory of radiationQuantum theory of radiation
Quantum theory of radiation
Β 
Atomic structure presentation
Atomic structure presentationAtomic structure presentation
Atomic structure presentation
Β 
Statistical Physics Assignment Help
Statistical Physics Assignment HelpStatistical Physics Assignment Help
Statistical Physics Assignment Help
Β 
statistical physics assignment help
statistical physics assignment helpstatistical physics assignment help
statistical physics assignment help
Β 
Quantum mechanics S5
Quantum mechanics S5 Quantum mechanics S5
Quantum mechanics S5
Β 
Phys2 ch4-kineticsgas
Phys2 ch4-kineticsgasPhys2 ch4-kineticsgas
Phys2 ch4-kineticsgas
Β 
Med.physics dr. ismail atomic and nuclear physics
Med.physics  dr. ismail atomic and nuclear physics Med.physics  dr. ismail atomic and nuclear physics
Med.physics dr. ismail atomic and nuclear physics
Β 
Phys201 3rd
Phys201 3rdPhys201 3rd
Phys201 3rd
Β 
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiationPHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
Β 
Quantum Mechanics Presentation
Quantum Mechanics PresentationQuantum Mechanics Presentation
Quantum Mechanics Presentation
Β 
General Chemistry I - CHEM 181Critical Thinking Exercise.docx
General Chemistry I - CHEM 181Critical Thinking Exercise.docxGeneral Chemistry I - CHEM 181Critical Thinking Exercise.docx
General Chemistry I - CHEM 181Critical Thinking Exercise.docx
Β 
Chapter-2-Prof-N.M.pptx
Chapter-2-Prof-N.M.pptxChapter-2-Prof-N.M.pptx
Chapter-2-Prof-N.M.pptx
Β 
IIT JEE Physics 1995
IIT JEE Physics   1995IIT JEE Physics   1995
IIT JEE Physics 1995
Β 
Radiation lecture 1 nov 2013
Radiation lecture 1 nov 2013Radiation lecture 1 nov 2013
Radiation lecture 1 nov 2013
Β 
Modern physics
Modern physicsModern physics
Modern physics
Β 
CBSE Class 11 Chemistry Sample ebook
CBSE Class 11 Chemistry Sample ebookCBSE Class 11 Chemistry Sample ebook
CBSE Class 11 Chemistry Sample ebook
Β 
Stellar evolution 2015
Stellar evolution 2015Stellar evolution 2015
Stellar evolution 2015
Β 
Radiavtive Heat Transfer assignment
Radiavtive Heat Transfer assignmentRadiavtive Heat Transfer assignment
Radiavtive Heat Transfer assignment
Β 
Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)
Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)
Definitions and MCQs of Ninth Class Chemistry (Atomic Structure)
Β 

More from Pooja M

Chapter 1 - Unit s and Measurement.pptx
Chapter 1 - Unit s and Measurement.pptxChapter 1 - Unit s and Measurement.pptx
Chapter 1 - Unit s and Measurement.pptxPooja M
Β 
Chapter 2 - Mechanical Properties of Fluids.pptx
Chapter 2 - Mechanical Properties of Fluids.pptxChapter 2 - Mechanical Properties of Fluids.pptx
Chapter 2 - Mechanical Properties of Fluids.pptxPooja M
Β 
Chapter 1 - Rotational Dynamics.pptx
Chapter 1 - Rotational Dynamics.pptxChapter 1 - Rotational Dynamics.pptx
Chapter 1 - Rotational Dynamics.pptxPooja M
Β 
Thermodynamics.ppt
Thermodynamics.pptThermodynamics.ppt
Thermodynamics.pptPooja M
Β 
Chapter 5 - Oscillation.pptx
Chapter 5 - Oscillation.pptxChapter 5 - Oscillation.pptx
Chapter 5 - Oscillation.pptxPooja M
Β 
Chapter 6 - Superposition of waves.pptx
Chapter 6 - Superposition of waves.pptxChapter 6 - Superposition of waves.pptx
Chapter 6 - Superposition of waves.pptxPooja M
Β 
Chapter 7 - Wave optics.pptx
Chapter 7 - Wave optics.pptxChapter 7 - Wave optics.pptx
Chapter 7 - Wave optics.pptxPooja M
Β 
Chapter 8 - Electrostatic.pptx
Chapter 8 - Electrostatic.pptxChapter 8 - Electrostatic.pptx
Chapter 8 - Electrostatic.pptxPooja M
Β 
Current Electricity.pptx
Current Electricity.pptxCurrent Electricity.pptx
Current Electricity.pptxPooja M
Β 
Chap 11 - Magnetic Materials.pptx
Chap 11 - Magnetic Materials.pptxChap 11 - Magnetic Materials.pptx
Chap 11 - Magnetic Materials.pptxPooja M
Β 
Chap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptx
Chap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptxChap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptx
Chap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptxPooja M
Β 
Chapter 16 - Semiconductor Devices.pptx
Chapter 16 - Semiconductor Devices.pptxChapter 16 - Semiconductor Devices.pptx
Chapter 16 - Semiconductor Devices.pptxPooja M
Β 
Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)
Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)
Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)Pooja M
Β 
CLASS XI - Chapter 9 optics (MAHARASHRA STATE BOARD)
CLASS XI - Chapter 9   optics  (MAHARASHRA STATE BOARD)CLASS XI - Chapter 9   optics  (MAHARASHRA STATE BOARD)
CLASS XI - Chapter 9 optics (MAHARASHRA STATE BOARD)Pooja M
Β 
CLASSXII (PHYSICS) Chapter 10 electrostatics
CLASSXII (PHYSICS) Chapter 10   electrostaticsCLASSXII (PHYSICS) Chapter 10   electrostatics
CLASSXII (PHYSICS) Chapter 10 electrostaticsPooja M
Β 
PHYSICS CLASS XI Chapter 5 - gravitation
PHYSICS CLASS XI Chapter 5 - gravitationPHYSICS CLASS XI Chapter 5 - gravitation
PHYSICS CLASS XI Chapter 5 - gravitationPooja M
Β 
Chapter 4 laws of motion
Chapter 4   laws of motion Chapter 4   laws of motion
Chapter 4 laws of motion Pooja M
Β 
Chapter 2 mechanical properties of fluids
Chapter 2   mechanical properties of fluids Chapter 2   mechanical properties of fluids
Chapter 2 mechanical properties of fluids Pooja M
Β 
Chapter 3 motion in a plane
Chapter 3   motion in a plane Chapter 3   motion in a plane
Chapter 3 motion in a plane Pooja M
Β 
Current electricity print quizizz
Current electricity   print   quizizzCurrent electricity   print   quizizz
Current electricity print quizizzPooja M
Β 

More from Pooja M (20)

Chapter 1 - Unit s and Measurement.pptx
Chapter 1 - Unit s and Measurement.pptxChapter 1 - Unit s and Measurement.pptx
Chapter 1 - Unit s and Measurement.pptx
Β 
Chapter 2 - Mechanical Properties of Fluids.pptx
Chapter 2 - Mechanical Properties of Fluids.pptxChapter 2 - Mechanical Properties of Fluids.pptx
Chapter 2 - Mechanical Properties of Fluids.pptx
Β 
Chapter 1 - Rotational Dynamics.pptx
Chapter 1 - Rotational Dynamics.pptxChapter 1 - Rotational Dynamics.pptx
Chapter 1 - Rotational Dynamics.pptx
Β 
Thermodynamics.ppt
Thermodynamics.pptThermodynamics.ppt
Thermodynamics.ppt
Β 
Chapter 5 - Oscillation.pptx
Chapter 5 - Oscillation.pptxChapter 5 - Oscillation.pptx
Chapter 5 - Oscillation.pptx
Β 
Chapter 6 - Superposition of waves.pptx
Chapter 6 - Superposition of waves.pptxChapter 6 - Superposition of waves.pptx
Chapter 6 - Superposition of waves.pptx
Β 
Chapter 7 - Wave optics.pptx
Chapter 7 - Wave optics.pptxChapter 7 - Wave optics.pptx
Chapter 7 - Wave optics.pptx
Β 
Chapter 8 - Electrostatic.pptx
Chapter 8 - Electrostatic.pptxChapter 8 - Electrostatic.pptx
Chapter 8 - Electrostatic.pptx
Β 
Current Electricity.pptx
Current Electricity.pptxCurrent Electricity.pptx
Current Electricity.pptx
Β 
Chap 11 - Magnetic Materials.pptx
Chap 11 - Magnetic Materials.pptxChap 11 - Magnetic Materials.pptx
Chap 11 - Magnetic Materials.pptx
Β 
Chap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptx
Chap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptxChap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptx
Chap 11 - ELECTRIC CURRENT THROUGH CONDUCTOR.pptx
Β 
Chapter 16 - Semiconductor Devices.pptx
Chapter 16 - Semiconductor Devices.pptxChapter 16 - Semiconductor Devices.pptx
Chapter 16 - Semiconductor Devices.pptx
Β 
Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)
Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)
Chapter 9 - Prism, optical instruments (PHYSICS - CLASS XI)
Β 
CLASS XI - Chapter 9 optics (MAHARASHRA STATE BOARD)
CLASS XI - Chapter 9   optics  (MAHARASHRA STATE BOARD)CLASS XI - Chapter 9   optics  (MAHARASHRA STATE BOARD)
CLASS XI - Chapter 9 optics (MAHARASHRA STATE BOARD)
Β 
CLASSXII (PHYSICS) Chapter 10 electrostatics
CLASSXII (PHYSICS) Chapter 10   electrostaticsCLASSXII (PHYSICS) Chapter 10   electrostatics
CLASSXII (PHYSICS) Chapter 10 electrostatics
Β 
PHYSICS CLASS XI Chapter 5 - gravitation
PHYSICS CLASS XI Chapter 5 - gravitationPHYSICS CLASS XI Chapter 5 - gravitation
PHYSICS CLASS XI Chapter 5 - gravitation
Β 
Chapter 4 laws of motion
Chapter 4   laws of motion Chapter 4   laws of motion
Chapter 4 laws of motion
Β 
Chapter 2 mechanical properties of fluids
Chapter 2   mechanical properties of fluids Chapter 2   mechanical properties of fluids
Chapter 2 mechanical properties of fluids
Β 
Chapter 3 motion in a plane
Chapter 3   motion in a plane Chapter 3   motion in a plane
Chapter 3 motion in a plane
Β 
Current electricity print quizizz
Current electricity   print   quizizzCurrent electricity   print   quizizz
Current electricity print quizizz
Β 

Recently uploaded

call girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈ
call girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈcall girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈ
call girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈ9953056974 Low Rate Call Girls In Saket, Delhi NCR
Β 
Class 11 Legal Studies Ch-1 Concept of State .pdf
Class 11 Legal Studies Ch-1 Concept of State .pdfClass 11 Legal Studies Ch-1 Concept of State .pdf
Class 11 Legal Studies Ch-1 Concept of State .pdfakmcokerachita
Β 
Hybridoma Technology ( Production , Purification , and Application )
Hybridoma Technology  ( Production , Purification , and Application  ) Hybridoma Technology  ( Production , Purification , and Application  )
Hybridoma Technology ( Production , Purification , and Application ) Sakshi Ghasle
Β 
β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...
β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...
β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...Marc Dusseiller Dusjagr
Β 
The Most Excellent Way | 1 Corinthians 13
The Most Excellent Way | 1 Corinthians 13The Most Excellent Way | 1 Corinthians 13
The Most Excellent Way | 1 Corinthians 13Steve Thomason
Β 
The basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptxThe basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptxheathfieldcps1
Β 
Alper Gobel In Media Res Media Component
Alper Gobel In Media Res Media ComponentAlper Gobel In Media Res Media Component
Alper Gobel In Media Res Media ComponentInMediaRes1
Β 
Incoming and Outgoing Shipments in 1 STEP Using Odoo 17
Incoming and Outgoing Shipments in 1 STEP Using Odoo 17Incoming and Outgoing Shipments in 1 STEP Using Odoo 17
Incoming and Outgoing Shipments in 1 STEP Using Odoo 17Celine George
Β 
Accessible design: Minimum effort, maximum impact
Accessible design: Minimum effort, maximum impactAccessible design: Minimum effort, maximum impact
Accessible design: Minimum effort, maximum impactdawncurless
Β 
BASLIQ CURRENT LOOKBOOK LOOKBOOK(1) (1).pdf
BASLIQ CURRENT LOOKBOOK  LOOKBOOK(1) (1).pdfBASLIQ CURRENT LOOKBOOK  LOOKBOOK(1) (1).pdf
BASLIQ CURRENT LOOKBOOK LOOKBOOK(1) (1).pdfSoniaTolstoy
Β 
CARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptxCARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptxGaneshChakor2
Β 
Science 7 - LAND and SEA BREEZE and its Characteristics
Science 7 - LAND and SEA BREEZE and its CharacteristicsScience 7 - LAND and SEA BREEZE and its Characteristics
Science 7 - LAND and SEA BREEZE and its CharacteristicsKarinaGenton
Β 
18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdfssuser54595a
Β 
Sanyam Choudhary Chemistry practical.pdf
Sanyam Choudhary Chemistry practical.pdfSanyam Choudhary Chemistry practical.pdf
Sanyam Choudhary Chemistry practical.pdfsanyamsingh5019
Β 
_Math 4-Q4 Week 5.pptx Steps in Collecting Data
_Math 4-Q4 Week 5.pptx Steps in Collecting Data_Math 4-Q4 Week 5.pptx Steps in Collecting Data
_Math 4-Q4 Week 5.pptx Steps in Collecting DataJhengPantaleon
Β 
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Sapana Sha
Β 
KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...
KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...
KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...M56BOOKSTORE PRODUCT/SERVICE
Β 

Recently uploaded (20)

call girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈ
call girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈcall girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈ
call girls in Kamla Market (DELHI) πŸ” >ΰΌ’9953330565πŸ” genuine Escort Service πŸ”βœ”οΈβœ”οΈ
Β 
Class 11 Legal Studies Ch-1 Concept of State .pdf
Class 11 Legal Studies Ch-1 Concept of State .pdfClass 11 Legal Studies Ch-1 Concept of State .pdf
Class 11 Legal Studies Ch-1 Concept of State .pdf
Β 
Hybridoma Technology ( Production , Purification , and Application )
Hybridoma Technology  ( Production , Purification , and Application  ) Hybridoma Technology  ( Production , Purification , and Application  )
Hybridoma Technology ( Production , Purification , and Application )
Β 
β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...
β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...
β€œOh GOSH! Reflecting on Hackteria's Collaborative Practices in a Global Do-It...
Β 
The Most Excellent Way | 1 Corinthians 13
The Most Excellent Way | 1 Corinthians 13The Most Excellent Way | 1 Corinthians 13
The Most Excellent Way | 1 Corinthians 13
Β 
The basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptxThe basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptx
Β 
Alper Gobel In Media Res Media Component
Alper Gobel In Media Res Media ComponentAlper Gobel In Media Res Media Component
Alper Gobel In Media Res Media Component
Β 
Incoming and Outgoing Shipments in 1 STEP Using Odoo 17
Incoming and Outgoing Shipments in 1 STEP Using Odoo 17Incoming and Outgoing Shipments in 1 STEP Using Odoo 17
Incoming and Outgoing Shipments in 1 STEP Using Odoo 17
Β 
TataKelola dan KamSiber Kecerdasan Buatan v022.pdf
TataKelola dan KamSiber Kecerdasan Buatan v022.pdfTataKelola dan KamSiber Kecerdasan Buatan v022.pdf
TataKelola dan KamSiber Kecerdasan Buatan v022.pdf
Β 
Accessible design: Minimum effort, maximum impact
Accessible design: Minimum effort, maximum impactAccessible design: Minimum effort, maximum impact
Accessible design: Minimum effort, maximum impact
Β 
BASLIQ CURRENT LOOKBOOK LOOKBOOK(1) (1).pdf
BASLIQ CURRENT LOOKBOOK  LOOKBOOK(1) (1).pdfBASLIQ CURRENT LOOKBOOK  LOOKBOOK(1) (1).pdf
BASLIQ CURRENT LOOKBOOK LOOKBOOK(1) (1).pdf
Β 
CARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptxCARE OF CHILD IN INCUBATOR..........pptx
CARE OF CHILD IN INCUBATOR..........pptx
Β 
Science 7 - LAND and SEA BREEZE and its Characteristics
Science 7 - LAND and SEA BREEZE and its CharacteristicsScience 7 - LAND and SEA BREEZE and its Characteristics
Science 7 - LAND and SEA BREEZE and its Characteristics
Β 
18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf
18-04-UA_REPORT_MEDIALITERAΠ‘Y_INDEX-DM_23-1-final-eng.pdf
Β 
Sanyam Choudhary Chemistry practical.pdf
Sanyam Choudhary Chemistry practical.pdfSanyam Choudhary Chemistry practical.pdf
Sanyam Choudhary Chemistry practical.pdf
Β 
Model Call Girl in Tilak Nagar Delhi reach out to us at πŸ”9953056974πŸ”
Model Call Girl in Tilak Nagar Delhi reach out to us at πŸ”9953056974πŸ”Model Call Girl in Tilak Nagar Delhi reach out to us at πŸ”9953056974πŸ”
Model Call Girl in Tilak Nagar Delhi reach out to us at πŸ”9953056974πŸ”
Β 
_Math 4-Q4 Week 5.pptx Steps in Collecting Data
_Math 4-Q4 Week 5.pptx Steps in Collecting Data_Math 4-Q4 Week 5.pptx Steps in Collecting Data
_Math 4-Q4 Week 5.pptx Steps in Collecting Data
Β 
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Β 
Staff of Color (SOC) Retention Efforts DDSD
Staff of Color (SOC) Retention Efforts DDSDStaff of Color (SOC) Retention Efforts DDSD
Staff of Color (SOC) Retention Efforts DDSD
Β 
KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...
KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...
KSHARA STURA .pptx---KSHARA KARMA THERAPY (CAUSTIC THERAPY)β€”β€”β€”β€”IMP.OF KSHARA ...
Β 

Chapter 3 - Kinetic theory of gases and radiation exercises solution

  • 1. 1 CLASS XII PHYSICS CHAPTER 3 KINETIC THEORY OF GASES AND RADIATION Exercises
  • 2. 2 Kinetic Theory of Gases and Radiation 1. Choose the correct option: i) In an ideal gas, the molecules possess (A) only kinetic energy (B) both kinetic energy and potential energy (C) only potential energy (D) neither kinetic energy nor potential energy ii) The mean free path Ξ» of molecules is given by where n is the number of molecules per unit volume and d is the diameter of the molecules. (A) √ 2 πœ‹ 𝑛 𝑑2 (B) 1 πœ‹ 𝑛 𝑑2 (C) 1 √2 πœ‹ 𝑛 𝑑2 (D) 1 √2 πœ‹ 𝑛 𝑑 iii) If the pressure of an ideal gas decreases by 10% isothermally, then its volume will _______. (A) decrease by 9% (B) increase by 9% (C) decrease by 10% (D) increase by 11.11% iv) If a = 0.72 and r = 0.24, then the value of π‘‘π‘Ÿ is (A) 0.02 (B) 0.04 (C) 0.4 (D) 0.2 v) The ratio of emissive power of perfect blackbody at 1327Β°C and 527Β°C is (A) 4:1 (B) 16:1 (C) 2:1 (D) 8:1 2. Answer in brief: i) What will happen to the mean square speed of the molecules of a gas if the temperature of the gas increases? Ans: If the temperature of a gas increases, the mean square speed of the molecules of the gas will increase in the same proportion. ii) On what factors do the degrees of freedom depend? Ans: The degrees of freedom depend upon (i) the number of atoms forming a molecule (ii) the structure of the molecule (iii) the temperature of the gas. iii) Write ideal gas equation for a mass of 7 g of nitrogen gas. Ans:
  • 3. 3 iv) If the density of oxygen is 1.44 kg/π‘š3 at a pressure of 105 N/π‘š2 , find the root mean square velocity of oxygen molecules. Ans: v) Define athermanous substances and diathermanous substances. Ans: Athermanous substances Substances that don't allow transmission of infrared radiation through them are called athermanous substances. - For example, wood, metal, 𝐢𝑂2, water vapours, etc. Diathermanous substances Substances that allow transmission of infrared radiation through them are called diathermanous substances. - For example, rock salt, pure air, glass, etc. 3. When a gas is heated, its temperature increases. Explain this phenomenon on the basis of the kinetic theory of gases. Ans: Molecules of a gas are in a state of continuous random motion. They possess kinetic energy. When a gas is heated, there is an increase in the average kinetic energy per molecule of the gas. Hence, its temperature increases (the average kinetic energy per molecule being proportional to the absolute temperature of the gas). 4. Explain, on the basis of the kinetic theory of gases, how the pressure of a gas changes if its volume is reduced at a constant temperature. Ans: The average kinetic energy per molecule of a gas is constant at a constant temperature. When the volume of a gas is reduced at a constant temperature, the number of collisions of gas molecules per unit time with the walls of the container increases. This increases the momentum transferred per unit time per unit area, i.e., the force exerted by the gas on the walls. Hence, the pressure of the gas increases.
  • 4. 4 5. Mention the conditions under which a real gas obeys ideal gas equation. Ans: A real gas obeys the ideal gas equation when the temperature is very high and pressure is very low [Note: Under these conditions, the density of a gas is very low. Hence, the molecules, on average, are far away from each other. The intermolecular forces are then not of much consequence.] 6. State the law of equipartition of energy and hence calculate the molar specific heat of monatomic and diatomic gases at constant volume and constant pressure. Ans:
  • 5. 5 7. What is a perfect blackbody? How can it be realized in practice? Ans: A perfect blackbody or simply a blackbody is defined as a body which absorbs all the radiant energy incident on it. Fery designed a spherical blackbody which consists of a hollow double-walled, metallic sphere provided with a tiny hole or aperture on one side, Fig. The inside wall of the sphere is blackened with lampblack while the outside is silver-plated. The space between the two walls is evacuated to minimize heat loss by conduction and convection. Any radiation entering the sphere through the aperture suffers multiple reflections where about 97% of it is absorbed in each incidence by the coating of lampblack. The radiation is almost completely absorbed after a number of internal reflections. A conical projection on the inside wall opposite the hole minimizes the probability of incident radiation escaping out. When the sphere is placed in a bath of suitable fused salts, so as to maintain it at the desired temperature, the hole serves as a source of black-body radiation. The intensity and the nature of the radiation depend only on the temperature of the walls.
  • 6. 6 A blackbody, by definition, has a coefficient of absorption equal to 1. Hence, its coefficient of reflection and coefficient of transmission are both zero. The radiation from a blackbody, called blackbody radiation, covers the entire range of the electromagnetic spectrum. Hence, a blackbody is called a full radiator. 8. State (i) Stefan-Boltzmann law. Ans: (ii) Wien's displacement law Ans: 9. Explain the spectral distribution of blackbody radiation. Ans: i. The rate of emission per unit area or power per unit area of a surface is defined as a function of the wavelength Ξ» of the emitted radiation. ii. Scientists studied the energy distribution of blackbody radiation as a function of wavelength. iii. By keeping the source of radiation (such as a cavity radiator) at different temperatures they measured the radiant power corresponding to different wavelengths. The measurements were represented graphically in the form of curves showing the variation of radiant power per unit area as a function of wavelength Ξ» at different constant temperatures as shown in the figure. 10. Prove Kirchhoff’s law of radiation theoretically.
  • 7. 7 Ans: Consider an ordinary body O and perfectly black body B of the same dimension suspended in a uniform temperature enclosure as shown in the figure. At thermal equilibrium, both the bodies will have the same temperature as that of the enclosure. Let, E = emissive power of ordinary body O Eb = emissive power of perfectly black body B a = coefficient of absorption of O e = emissivity of O Q = radiant energy incident per unit time per unit area on each body. Quantity of heat absorbed per unit area per unit time by body O = aQ. Quantity of heat energy emitted per unit area per unit time by body O = E. Since there is no change in temperature E = aQ Q = E/a .…(1) Quantity of heat absorbed per unit area per unit time by a perfectly black body, B = Q The radiant heat energy emitted per unit time per unit area by a perfectly black body, B = Eb Since there is no change in temperature. Eb = Q .…(2) From equations (1) and (2), 11. Calculate the ratio of the mean square speeds of molecules of a gas at 30 K and 120 K. Ans:
  • 8. 8 12. Two vessels A and B are filled with the same gas where the volume, temperature, and pressure in vessel A is twice the volume, temperature, and pressure in vessel B. Calculate the ratio of the number of molecules of the gas in vessel A to that in vessel B. Ans: 13. A gas in a cylinder is at pressure P. If the masses of all the molecules are made one-third of their original value and their speeds are doubled, then find the resultant pressure. Ans: 14. Show that rms velocity of an oxygen molecule is √2 times that of a sulfur dioxide molecule at S.T.P. Ans:
  • 9. 9 15. At what temperature will oxygen molecules have same rms speed as helium molecules at S.T.P.? (Molecular masses of oxygen and helium are 32 and 4 respectively). Ans: 16. Compare the rms speed of hydrogen molecules at 127℃ with rms speed of oxygen molecules at 27℃ given that molecular masses of hydrogen and oxygen are 2 and 32 respectively. Ans:
  • 10. 10 17. Find the kinetic energy of 5 litre of a gas at STP given the standard pressure is 1.013 Γ— 105 N/π‘š2 . Ans: 18. Calculate the average molecular kinetic energy (i) per kmol (ii) per kg (iii) per molecule of oxygen at 127Β°C, given that the molecular weight of oxygen is 32, R is 8.31 J π‘šπ‘œπ‘™βˆ’1 πΎβˆ’1 and Avogadro’s number 𝑁𝐴 is 6.02 Γ— 1023 molecules π‘šπ‘œπ‘™βˆ’1 . Ans:
  • 11. 11 19. Calculate the energy radiated in one minute by a blackbody of surface area 100 π‘π‘š2 when it is maintained at 227Β°C. Ans: 20. Energy is emitted from a hole in an electric furnace at the rate of 20 W, when the temperature of the furnace is 727Β°C. What is the area of the hole? (Take Stefan’s constant Οƒ to be 5.7 Γ— 10βˆ’8 𝐽 π‘ βˆ’1 π‘šβˆ’2 πΎβˆ’4 ) Ans:
  • 12. 12 21. The emissive power of a sphere of area 0.02 π‘š2 is 0.5 kcal π‘ βˆ’1 π‘šβˆ’2 . What is the amount of heat radiated by the spherical surface in 20 seconds? Ans: 22. Compare the rates of emission of heat by a blackbody maintained at 727Β°C and at 227Β°C, if the black bodies are surrounded by an enclosure (black) at 27Β°C. What would be the ratio of their rates of loss of heat? Ans:
  • 13. 13 23. The earth’s mean temperature can be assumed to be 280 K. How will the curve of blackbody radiation look like for this temperature? Find out πœ†π‘šπ‘Žπ‘₯. In which part of the electromagnetic spectrum, does this value lie? Ans: 24. A small blackened solid copper sphere of radius 2.5 cm is placed in an evacuated chamber. The temperature of the chamber is maintained at 100 Β°C. At what rate must energy be supplied to the copper sphere to maintain its temperature at 110 Β°C? (Take Stefan’s constant Οƒ to be 5.67 Γ— 10βˆ’8 𝐽 π‘ βˆ’1 π‘šβˆ’2 πΎβˆ’4 and treat the sphere as a blackbody.) Ans:
  • 14. 14 25. Find the temperature of a blackbody if its spectrum has a peak at (a) πœ†π‘šπ‘Žπ‘₯ = 700 nm (visible), (b) πœ†π‘šπ‘Žπ‘₯= 3 cm (microwave region) (c) Ξ»max = 3 cm (FM radio waves). (Take Wien’s constant b = 2.897 Γ— 10βˆ’3 m K). Ans: