fiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES Kinetic Theory, Thermodynamics OBJECTIVE QUESTIONS IIT-JAM-2005
|
|
- Rosemary McLaughlin
- 6 years ago
- Views:
Transcription
1 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES Kinetic heory, hermodynamics OBJEIE QUESIONS II-JAM Q. he molar specific heat of a gas as given from the kinetic theory is R. If it is not specified whether it is or, one could conclude that the molecules of the gas (a) are definitely monatomic (b) are definitely rigid diatomic are definitely non-rigid diatomic (d) can be monatomic or rigid diatomic Ans. : (d) 5R Solution: If molecule is mono atomic then p = and if molecule is rigid diatomic then 5R =. Q. he value of entropy at absolute zero of temperature would be (a) zero for all the materials (b) finite for all the materials zero for some materials and non-zero for others (d) unpredictable for any material Solution: If system will achieve absolute zero then it is perfectly ordered system then entropy will be zero. Q. Which of the following statements is INORRE? (a) Indistinguishable particles obey Maxwell-Boltzmann statistics (b) All particles of an ideal Bose gas occupy a single energy state at = 0 he integral spin particles obey Bose-Einstein statistics (d) rotons obey Fermi-Dirac statistics Solution: Distinguishable particles obey Maxwell-Boltzmann statistics. Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 9
2 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES II-JAM-006 Q4. A solid melts into a liquid via first order phase transition. he relationship between the pressure and the temperature of the phase transition is = - + 0, where 0 is a constant. he entropy change associated with the phase transition is.0 J mole - K -. he d lausius-lapeyron equation for the latent heat is L = Δv. Here Δ v = v liquid vsolid d is the change in molar volume at the phase transition. he correct statement relating the values of the volumes is (a) v = v (b) v v liquid solid liquid = solid v liquid = v solid (d) v quid = v solid + Ans. : Solution: Since = + 0 d = d d dl It is given L = Δv L= Δ v = Δ v d d - - Since ds =.0 Jmole K.0 J mole - K - dq mdl ds = = d = = Δv Δ v= II-JAM-007 Q5. Experimental measurements of heat capacity per mole of Aluminum at low temperatures show that the data can be fitted to the formula, = a + b, where a = JK - mole -, b =.48 x 0-5 JK -4 mole - and is the temperature in in Kelvin. he entropy of a mole of Aluminum at such temperatures is given by the formula b a b (a) a + + c, where c > 0 is a constant (b) + + c, where c > 0 is a constant 4 b a + (d) a b + 4 Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 9
3 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES Solution: cd v ds = s= a + b d b = + + a c II-JAM-008 Q6. he chemical potential of an ideal Bose gas at any temperature is (a) necessarily negative (b) either zero or negative necessarily positive (d) either zero or positive Ans. : (b) Solution: he chemical potential of an ideal Bose gas at any temperature is either zero or negative.(zero in case of photon ). Q7. A thermodynamic system is maintained at constant temperature and pressure. In thermodynamic equilibrium, its (a) Gibbs free energy is minimum (b) enthalpy is maximum Helmholtz free energy is minimum (d) internal energy is zero Solution: A thermodynamic system is maintained at constant temperature and pressure can be defined by Gibbs energy dg = Sd + d 0 i.e. Gibbs free energy is minimum. II-JAM-009 Q8. A box containing moles of a diatomic ideal gas at temperature 0 is connected to another identical box containing moles of a monatomic ideal gas at temperature 5 0. here are no thermal losses and the heat capacity of the boxes is negligible. Find the final temperature of the mixture of gases (ignore the vibrational degrees of freedom for the diatomic molecules). (a) 0 (b) (d) 0 Ans. : Solution: Internal energy of the system remains conserve i.e. Umonoatomic + Udiatomic = Umixture Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 94
4 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES U monotomic = n, U diatomic = n 5R R v =, v =, n = n =, 0 =, = 50 n + n Let the common temperature of mixture is and specific heat is = n + n and number of moles of mixture is n= n+ n, then n + n = n =.5 0 Q9. Isothermal compressibility κ of a substance is defined asκ Ans. : Solution: moles of an ideal gas will be n (a) (b) = nr and k = =. II-JAM-00 = (d) n. Its value for n Q0. A gas of molecules each having mass m is in thermal equilibrium at a temperature. Let v x, v y, v z be the artesian components of velocity, v, of a molecules. he mean value of ( v α v + β v ) x y z is k (a) ( α + β ) B m k + (b) ( α + β ) B m ( k ) B m β α k (d) ( α + β ) B m Solution: ( ) v αv + βv = v + α v + β v αv v + βv v βαv v x y z x y y x y z x y z ( ) v αv + βv = v + α v + β v α v v + β v v βα v v x y z x y y x y z x y z Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 95
5 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES k B vx = vy = vz = and vx = vy = vz = 0 m k B ( vx αvy + βvz) = ( + α + β ) m Q. A trapped air bubble of volume 0 is released from a depth h measured from the water surface in a large water tank. he volume of the bubble grows to 0 as it reaches just below the surface. he temperature of the water and the pressure above the surface of water (0 5 N/m ) remain constant throughout the process. If the density of water is 000 kg/ m and the acceleration due to gravity is 0m/ s, then the depth h is (a) m (b) 0 m 50 m (d) 00 m Ans. : (b) Solution: At depth h pressure = 0 + ρgh and volume = 0 where At surface pressure = 0 and volume = 0 ( ρ ) + gh = = 0 N / m, g = 0 m/ s h= 0m ρ = 000 kg / m II-JAM-0 Q. onsider free expansion of one mole of an ideal gas in an adiabatic container from volume to. he entropy change of the gas, calculated by considering a reversible process between the original state( ) to the final state ( ) where is the, temperature of the system is denoted by Δ S. he corresponding change in the entropy of the surrounding is Δ S. Which of the following combinations is correct? (a) Δ S = Rln ( / ), Δ S = Rln ( / ) (b) Δ S = Rln ( / ), Δ S = Rln ( / ) ( ) Δ S = Rln /, Δ S = 0 (d) ( ) Δ S = Rln /, Δ S = 0, Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 96
6 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES Ans. : Solution: Free expansion is irreversible process when gas expand to which can be explained by choosing any path between two state (because entropy is state function). So one can choose reversible isothermal process. So Δ S = Rln. Hence it is free expansion so entropy of surrounding is Δ S = 0. Q. A gas of molecular mass m is at temperature. If the gas obeys Maxwell-Boltzmann velocity distribution, the average speed of molecules is given by (a) k B k (b) B m m k B πm (d) 8k B Ans. : (d) II-JAM-0 Q4. For a liquid to vapour phase transition at tr, which of the following plots between specific Gibbs free energy g and temperature is correct? (a) g (b) g πm Liquid apour Liquid apour tr tr g (d) g Liquid apour Liquid apour tr tr Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 97
7 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES Q5. A tiny dust particle of mass kg is floating in air at 00K. Ignoring gravity, its rms speed (in µm/s) due to random collisions with air molecules will be closest to (a) 0. (b) 0 (d) 00 Ans. : Solution: v rms k = = = 0 0 m/ s m.4 0 Q6. When the temperature of a blackbody is doubled, the maximum value of its spectral energy density, with respect to that at initial temperature, would become (a) times (b) 8 times 6 times (d) times U Solution: U = U = U = 64U 4 4 U II-JAM-0 Q7. A blackbody at temperature emits radiation at a peak wavelength λ. If the temperature of the blackbody becomes 4, the new peak wavelength is (a) λ 56 Ans. : (d) (b) λ 64 λ 6 λmax λ λ Solution: From wein Law λmax = λmax λmax = = = 4 4 Q8. Let N MB, N BE, N FD denote the number of ways in which two particles can be distributed in two energy states according to Maxwell-Boltzmann, Bose-Einstein and Fermi-Dirac statistics respectively. hen N : N : N is MB BE (a) 4 : : (b) 4 : : 4 : : (d) 4 : : Solution: N = g = n = FD (d) λ 4 Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 98
8 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES For Maxwell W N n = g = = n 4 For boson N = g = n = ; W n+ g + = = = ng For Fermion N = g = n = ; g W = = = gg n Q9. wo thermally isolated identical systems have heat capacities which vary as v = β (where β > 0 ). Initially one system is at 00 K and the other at 400 K. he systems are then brought into thermal contact and the combined system is allowed to reach thermal equilibrium. he final temperature of the combined system is. Ans. : Solution: here is not a unique value of temperature rather range of temperature he maximum temperature when work done is zero so dq+ dq = 0 4 max max max ( 00) ( 400) 4 4 mβ d + mβ d = 0 = max ( 00) + ( 400) 4 4 = max = 60K he minimum temperature system is when process is reversible so change in entropy of system is zero Δ S +Δ = min S0 0 mβ ( ) ( ) min mβ d + d = 0 min = = 5K min So 5K 60K Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 99
9 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES II-JAM-04 Q0. In - dimension, an ensemble of N classical particles has energy of the form x E = + kx. he average internal energy of the system at temperature is m (a) Nk B (b) Nk B Nk B (d) Nk B Ans. : (d) Q. A solid metallic cube of heat capacity S is at temperature 00 K. It is brought in contact with a reservoir at 600 K. If the heat transfer takes place only between the reservoir and the cube, the entropy change of the universe after reaching the thermal equilibrium is (a) 0.69 S (b) 0.54 S 0.7 S (d) 0.9 S Ans. : (d) Q. A real gas has specific volume v at temperature. Its coefficient of volume expansion and isothermal compressibility are α and k, respectively. Its molar specific heat at constant pressure p and molar specific heat at constant volume v are related as (a) = R (b) p v + p = v vα + k Ans. : p vα = v + (d) p = v k Q. At atmospheric pressure ( = 0 5 a), aluminium melts at 550 K. As it melts, its density decreases from 0 kg/m to.9 0 kg/m. Latent heat of fusion of aluminium is 4 0 J/kg. he melting point of aluminium at a pressure of 0 7 a is closest to (a) 55. K (b) 55.6 K K (d) K Ans. : (b) Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 00
10 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES II-JAM-05 Q4. A system consists of N number of particles, N >>. Each particle can have only one of the two energies E or + ε ( ε ) E > 0. If the system is in equilibrium at a temperature, the average number of particles with energy E is N N (a) (b) / k e ε + Ans. : (d) Solution: ( E E ) ( ε ) E+ E ε k k k N = Ne = e N = Ne N / k e ε + (d) k Ne ε / Q5. A rigid and thermally isolated tank is divided into two compartments of equal volume, separated by a thin membrane. One compartment contains one mole of an ideal gas A and the other compartment contains one mole of a different ideal gas B. he two gases are in thermal equilibrium at a temperature. If the membrane ruptures, the two gases mix. Assume that the gases are chemically inert. he change in the total entropy of the gases on mixing is (a) 0 (b) R ln ln (d) R ln Ans. : (d) Solution: For A, number of microstate after mixing is For A, number of microstate before mixing is A B Δ S = Rln Rln = Rln A Similarly, for B Δ S = Rln Δ S =Δ S +Δ S = Rln B Q6. A rigid triangular molecule consists of three non-collinear atoms joined by rigid rods. Ans. : A he constant pressure molar specific heat ( p ) of an ideal gas consisting of such molecules is (a) 6 R (b) 5 R 4 R (d) R Solution: D.O.F = 6 6R U U = = = R = + R= 4R B Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 0
11 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES SEION B: MSQ Q7. As shown in the diagram AB and D are two isotherms at temperatures and, respectively ( ) >. A and BD are two reversible adiabats. In this arnot cycle, which of the following statements are true? Q Q (a) = (b) he entropy of the source decreases he entropy of the system increases Q D (d) Work done by the system W = Q Q, (b) and (d) Q8. In the thermodynamic cycle shown in the figure, one mole of a monatomic ideal gas is taken through a cycle. AB is a reversible isothermal expansion at a temperature of 800 K in which the volume of the gas is doubled. B is an isobaric contraction to the original volume in which the temperature is reduced to00 K. A is a constant volume process in which the pressure and temperature return to their initial values. he A net amount of heat (in Joules) absorbed by the gas in one complete cycle is. Ans. : 45 Solution: rocess A B is isothermal expansion A A = 800 K, A, A and B = 800 K, B = A, B = rocess B is isobaric B olume A = B =, = A, = 00K A is Isochoric B Δ Q = nra ln = 460J A ressure A Q B Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 0
12 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES nγrδ γ Δ Q = nδ = = R γ ( γ ) R Δ Q = ( ) ( ) γ ( γ ) ( ) R = 500 = 694J otal heat exchange is Q+ Q + Q = 45 = 044J Q9. One gram of ice at 0 o is melted and heated to water at 9 o. Assume that the specific heat remains constant over the entire process. he latent heat of fusion of ice is 80 alories/gm. he entropy change in the process (in alories per degree) is. Ans. : 0.9 ML 80 0 d 0 Solution: Δ S = =, Δ S = M 7 Δ S =.ln 7 7 Δ S =Δ S+ΔS 80 0 Δ S = +.ln = = II-JAM-06 Q0. A spherical closed container with smooth inner wall contains a monoatomic ideal gas. If the collisions between the wall and the atoms are elastic, then the Maxwell speeddistribution function dnv dv for the atoms is best represented by: (a) (b) dn v dv 0 v dn v dv 0 v dn v dv (d) dn v dv Ans. : 0 v 0 v Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 0
13 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES dn Solution: mv v exp dv k Q. For an ideal gas, which one of the following S - diagram is valid? (a) Isochor S Isobar (b) Isobar S Isochor Isochor (d) Isochor Isobar Isobar S S S Solution: = = isochoric and isobaric plot. > from the slope of Sdiagram one can plot Q. If U, F, H and G represent internal energy, Helmholtz free energy enthalpy and Gibbs free energy respectively, then which one of the following is a correct thermodynamic relation? (a) du = d ds (b) dh = d + ds df = d + Sd (d) dg = d + Sd Ans. : (b) Solution: H = U + dh = du + d + d ds d + d + d dh = d + ds S Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 04
14 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES Q. One mole of an ideal gas with average molecular speed v 0 is kept in a container of fixed volume. If the temperature of the gas is increased such that the average speed gets doubled, then (a) the mean free path of the gas molecule will increase (b) the mean free path of the gas molecule will not change the mean free path of the gas molecule will decrease (d) the collision frequency of the gas molecule with wall of the container remains unchanged. Ans. : (b) Solution: For fixed volume if temperature is increased then pressure is also increased by same amount so mean free path with not change k λ = π d p Q4. he diagram below shows three possible paths for an ideal gas to reach the final state f from an initial state i. Which among f (a) he work done by the gas is maximum along path -. (b) Minimum change in the internal energy occurs along path -. Maximum heat transfer is for path - (d) Heat transfer is path independent Solution: work done is area under curve so it is maximum in path Hence change in internal energy is same in all path so heat exchange is also maximum in path the following statements ( s ) is (are) correct? Q5. A cylinder contains 6 g of O. he work done when the gas is compressed to 75% of the original volume at constant temperature of [Universal gas constant R 8. J / ( mole K) 6 n= = 0.5, = 00k Near II, Hauz Khas, New Delhi 6 hone: / = ] 0 7 is. J. 8 B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 05 i
15 Institute for NE/JRF, GAE, II JAM, JES, IFR and GRE in HYSIAL SIENES Ans. : d 75 Solution: W = d nr = nr ln = ln.75 = 58J 00 Q6. An aluminum plate of mass 0. kg at Ans. : is immersed in 0.5 litre of water at 0 0 kept inside an insulating container and is then removed. If the temperature of the water is found to be 0, then the temperature of the aluminum plate is 0 (he specific heat of water and aluminum are 400 J / kg respectively, the density of water is 000 kg / m ) Solution: M asa( a f ai ) MwSw( w f wi) K and 900 J / kg = ( 68) = ( 96 9) ( af 68) = 450 ( af 68) = = = = 67.6 af = 94.6 Q7. If there is a 0% decrease in the atmospheric pressure at a hill compared to the pressure Ans. : at sea level, then the change in the boiling point of water is. 0 (ake latent heat of vaporisation of water as 70 kj / kg and the change in the specific volume at the boiling point to be. m / kg) af K Solution: 5 v v 5 0 d d d L = = = = = d v v L 70 0 Near II, Hauz Khas, New Delhi 6 hone: / B/6, Jia Sarai, Near II Hauz Khas, New Delhi 6 fiziks.physics@gmail.com 06
fiziks Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES
Content-Thermodynamics & Statistical Mechanics 1. Kinetic theory of gases..(1-13) 1.1 Basic assumption of kinetic theory 1.1.1 Pressure exerted by a gas 1.2 Gas Law for Ideal gases: 1.2.1 Boyle s Law 1.2.2
More informationPhase Changes and Latent Heat
Review Questions Why can a person remove a piece of dry aluminum foil from a hot oven with bare fingers without getting burned, yet will be burned doing so if the foil is wet. Equal quantities of alcohol
More informationA thermodynamic system is taken from an initial state X along the path XYZX as shown in the PV-diagram.
AP Physics Multiple Choice Practice Thermodynamics 1. The maximum efficiency of a heat engine that operates between temperatures of 1500 K in the firing chamber and 600 K in the exhaust chamber is most
More informationThermodynamics & Statistical Mechanics
hysics GRE: hermodynamics & Statistical Mechanics G. J. Loges University of Rochester Dept. of hysics & Astronomy xkcd.com/66/ c Gregory Loges, 206 Contents Ensembles 2 Laws of hermodynamics 3 hermodynamic
More informationKinetic Theory continued
Chapter 12 Kinetic Theory continued 12.4 Kinetic Theory of Gases The particles are in constant, random motion, colliding with each other and with the walls of the container. Each collision changes the
More informationProcess Nature of Process
AP Physics Free Response Practice Thermodynamics 1983B. The pv-diagram above represents the states of an ideal gas during one cycle of operation of a reversible heat engine. The cycle consists of the following
More informationKinetic Theory continued
Chapter 12 Kinetic Theory continued 12.4 Kinetic Theory of Gases The particles are in constant, random motion, colliding with each other and with the walls of the container. Each collision changes the
More informationUnit 7 (B) Solid state Physics
Unit 7 (B) Solid state Physics hermal Properties of solids: Zeroth law of hermodynamics: If two bodies A and B are each separated in thermal equilibrium with the third body C, then A and B are also in
More informationHandout 12: Thermodynamics. Zeroth law of thermodynamics
1 Handout 12: Thermodynamics Zeroth law of thermodynamics When two objects with different temperature are brought into contact, heat flows from the hotter body to a cooler one Heat flows until the temperatures
More informationHandout 12: Thermodynamics. Zeroth law of thermodynamics
1 Handout 12: Thermodynamics Zeroth law of thermodynamics When two objects with different temperature are brought into contact, heat flows from the hotter body to a cooler one Heat flows until the temperatures
More informationChapter 10. Thermal Physics. Thermodynamic Quantities: Volume V and Mass Density ρ Pressure P Temperature T: Zeroth Law of Thermodynamics
Chapter 10 Thermal Physics Thermodynamic Quantities: Volume V and Mass Density ρ Pressure P Temperature T: Zeroth Law of Thermodynamics Temperature Scales Thermal Expansion of Solids and Liquids Ideal
More informationChapter 15 Thermal Properties of Matter
Chapter 15 Thermal Properties of Matter To understand the mole and Avogadro's number. To understand equations of state. To study the kinetic theory of ideal gas. To understand heat capacity. To learn and
More informationDownloaded from
Chapter 13 (Kinetic Theory) Q1. A cubic vessel (with face horizontal + vertical) contains an ideal gas at NTP. The vessel is being carried by a rocket which is moving at a speed of500 ms in vertical direction.
More informationTEST-11(Solution) TOPIC : HEAT COMPLETE 2400 = m 80 [ Q = ml]
entigrade emperature (º) emperature () ES-(Solution) OI : HE OMLEE 400 = m 80 [Q = ml] Q. If specific heat of a substance is infinite, it means- () Heat is given out () Heat is taken in () No change in
More informationThermal & Statistical Physics Study Questions for the Spring 2018 Department Exam December 6, 2017
Thermal & Statistical Physics Study Questions for the Spring 018 Department Exam December 6, 017 1. a. Define the chemical potential. Show that two systems are in diffusive equilibrium if 1. You may start
More informationHandout 11: Ideal gas, internal energy, work and heat. Ideal gas law
Handout : Ideal gas, internal energy, work and heat Ideal gas law For a gas at pressure p, volume V and absolute temperature T, ideal gas law states that pv = nrt, where n is the number of moles and R
More informationUNIVERSITY COLLEGE LONDON. University of London EXAMINATION FOR INTERNAL STUDENTS. For The Following Qualifications:-
UNIVERSITY COLLEGE LONDON University of London EXAMINATION FOR INTERNAL STUDENTS For The Following Qualifications:- B.Sc. M.Sci. Physics 1B28: Thermal Physics COURSE CODE : PHYSIB28 UNIT VALUE : 0.50 DATE
More informationFirst Law of Thermodynamics Second Law of Thermodynamics Mechanical Equivalent of Heat Zeroth Law of Thermodynamics Thermal Expansion of Solids
Slide 1 / 66 1 What is the name of the following statement: "When two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with each other"? A B C D E First Law
More information(a) How much work is done by the gas? (b) Assuming the gas behaves as an ideal gas, what is the final temperature? V γ+1 2 V γ+1 ) pdv = K 1 γ + 1
P340: hermodynamics and Statistical Physics, Exam#, Solution. (0 point) When gasoline explodes in an automobile cylinder, the temperature is about 2000 K, the pressure is is 8.0 0 5 Pa, and the volume
More informationCHAPTER 9 Statistical Physics
CHAPTER 9 Statistical Physics 9.1 9.2 9.3 9.4 9.5 9.6 9.7 Historical Overview Maxwell Velocity Distribution Equipartition Theorem Maxwell Speed Distribution Classical and Quantum Statistics Fermi-Dirac
More informationThermodynamics and Statistical Physics. Preliminary Ph.D. Qualifying Exam. Summer 2009
Thermodynamics and Statistical Physics Preliminary Ph.D. Qualifying Exam Summer 2009 (Choose 4 of the following 6 problems) -----------------------------------------------------------------------------------------------------------
More information(Heat capacity c is also called specific heat) this means that the heat capacity number c for water is 1 calorie/gram-k.
Lecture 23: Ideal Gas Law and The First Law of Thermodynamics 1 (REVIEW) Chapter 17: Heat Transfer Origin of the calorie unit A few hundred years ago when people were investigating heat and temperature
More informationTemperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines
Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines Zeroeth Law Two systems individually in thermal equilibrium with a third
More informationCHEM Thermodynamics. Entropy, S
hermodynamics Change in Change in Entropy, S Entropy, S Entropy is the measure of dispersal. he natural spontaneous direction of any process is toward greater dispersal of matter and of energy. Dispersal
More informationCh. 19: The Kinetic Theory of Gases
Ch. 19: The Kinetic Theory of Gases In this chapter we consider the physics of gases. If the atoms or molecules that make up a gas collide with the walls of their container, they exert a pressure p on
More informationLecture. Polymer Thermodynamics 0331 L First and Second Law of Thermodynamics
1 Prof. Dr. rer. nat. habil. S. Enders Faculty III for Process Science Institute of Chemical Engineering Department of hermodynamics Lecture Polymer hermodynamics 0331 L 337 2.1. First Law of hermodynamics
More informationStatistical Mechanics
Statistical Mechanics Newton's laws in principle tell us how anything works But in a system with many particles, the actual computations can become complicated. We will therefore be happy to get some 'average'
More informationCHAPTER 21 THE KINETIC THEORY OF GASES-PART? Wen-Bin Jian ( 簡紋濱 ) Department of Electrophysics National Chiao Tung University
CHAPTER 1 THE KINETIC THEORY OF GASES-PART? Wen-Bin Jian ( 簡紋濱 ) Department of Electrophysics National Chiao Tung University 1. Molecular Model of an Ideal Gas. Molar Specific Heat of an Ideal Gas. Adiabatic
More information18.13 Review & Summary
5/2/10 10:04 PM Print this page 18.13 Review & Summary Temperature; Thermometers Temperature is an SI base quantity related to our sense of hot and cold. It is measured with a thermometer, which contains
More informationAP PHYSICS 2 WHS-CH-15 Thermodynamics Show all your work, equations used, and box in your answers!
AP PHYSICS 2 WHS-CH-15 Thermodynamics Show all your work, equations used, and box in your answers! Nicolas Léonard Sadi Carnot (1796-1832) Sadi Carnot was a French military engineer and physicist, often
More informationEntropy & the Second Law of Thermodynamics
PHYS102 Previous Exam Problems CHAPTER 20 Entropy & the Second Law of Thermodynamics Entropy gases Entropy solids & liquids Heat engines Refrigerators Second law of thermodynamics 1. The efficiency of
More informationHandout 11: Ideal gas, internal energy, work and heat. Ideal gas law
Handout : Ideal gas, internal energy, work and heat Ideal gas law For a gas at pressure p, volume V and absolute temperature T, ideal gas law states that pv = nrt, where n is the number of moles and R
More information(2) The volume of molecules is negligible in comparison to the volume of gas. (3) Molecules of a gas moves randomly in all direction.
9.1 Kinetic Theory of Gases : Assumption (1) The molecules of a gas are identical, spherical and perfectly elastic point masses. (2) The volume of molecules is negligible in comparison to the volume of
More informationPHY214 Thermal & Kinetic Physics Duration: 2 hours 30 minutes
BSc Examination by course unit. Friday 5th May 01 10:00 1:30 PHY14 Thermal & Kinetic Physics Duration: hours 30 minutes YOU ARE NOT PERMITTED TO READ THE CONTENTS OF THIS QUESTION PAPER UNTIL INSTRUCTED
More informationUNIT # 06 THERMODYNAMICS EXERCISE # 1. T i. 1. m Zn
UNI # 6 HERMODYNMIS EXERISE #. m Zn.S Zn.( f i + m H O.S H O.( f i (6.8 gm (.4 J/g ( f + 8 gm (4. J/g ( f [(6.8 (.4 + 8(4.] f (6.8 (.4 ( + (8 (4. ( (6.8(.4( (8(4.( f 97. (6.8(.4 (8(4.. U q + w heat absorb
More informationPHYS102 Previous Exam Problems. Temperature, Heat & The First Law of Thermodynamics
PHYS102 Previous Exam Problems CHAPTER 18 Temperature, Heat & The First Law of Thermodynamics Equilibrium & temperature scales Thermal expansion Exchange of heat First law of thermodynamics Heat conduction
More informationMME 2010 METALLURGICAL THERMODYNAMICS II. Fundamentals of Thermodynamics for Systems of Constant Composition
MME 2010 METALLURGICAL THERMODYNAMICS II Fundamentals of Thermodynamics for Systems of Constant Composition Thermodynamics addresses two types of problems: 1- Computation of energy difference between two
More informationCHAPTER - 12 THERMODYNAMICS
CHAPER - HERMODYNAMICS ONE MARK QUESIONS. What is hermodynamics?. Mention the Macroscopic variables to specify the thermodynamics. 3. How does thermodynamics differ from Mechanics? 4. What is thermodynamic
More informationUNIVERSITY OF SOUTHAMPTON
UNIVERSITY OF SOUTHAMPTON PHYS1013W1 SEMESTER 2 EXAMINATION 2014-2015 ENERGY AND MATTER Duration: 120 MINS (2 hours) This paper contains 8 questions. Answers to Section A and Section B must be in separate
More informationChapter 10: Thermal Physics
Chapter 10: hermal Physics hermal physics is the study of emperature, Heat, and how these affect matter. hermal equilibrium eists when two objects in thermal contact with each other cease to echange energy.
More informationThermal Physics. Topics to be covered. Slide 2 / 105. Slide 1 / 105. Slide 3 / 105. Slide 4 / 105. Slide 5 / 105. Slide 6 / 105.
Slide 1 / 105 Slide 2 / 105 Topics to be covered Thermal Physics Temperature and Thermal quilibrium Gas Laws Internal nergy Heat Work Laws of Thermodynamics Heat ngines Slide 3 / 105 Thermodynamics System
More informationHEAT & THERMODYNAMICS
Einstein lasses, Unit No. 0, 03, ardhman Ring Road laza, ikas uri Extn., Outer Ring Road New Delhi 0 08, h. : 9369035, 857 HT HEAT & THERMODYNAMIS Syllabus : HEAT Heat, temperature, thermal expansion;
More informationPressure Volume Work 2
ressure olume Work Multi-stage Expansion 1 3 w= 4 5 ( ) + 3( 3 ) + 4( 4 3) + ( ) 1 5 5 4 Reversible Expansion Make steps so small that hen d 0, d 0 δ w= d ( ) = + d d int d int w= dw= d path 1 int For
More information1985B4. A kilogram sample of a material is initially a solid at a temperature of 20 C. Heat is added to the sample at a constant rate of 100
1985B4. A 0.020-kilogram sample of a material is initially a solid at a temperature of 20 C. Heat is added to the sample at a constant rate of 100 joules per second until the temperature increases to 60
More informationLecture 5. PHYC 161 Fall 2016
Lecture 5 PHYC 161 Fall 2016 Ch. 19 First Law of Thermodynamics In a thermodynamic process, changes occur in the state of the system. Careful of signs! Q is positive when heat flows into a system. W is
More information7. (2) Of these elements, which has the greatest number of atoms in a mole? a. hydrogen (H) b. oxygen (O) c. iron (Fe) d. gold (Au) e. all tie.
General Physics I Exam 5 - Chs. 13,14,15 - Heat, Kinetic Theory, Thermodynamics Dec. 14, 2010 Name Rec. Instr. Rec. Time For full credit, make your work clear to the grader. Show formulas used, essential
More informationUNIVESITY OF SWAZILAND FACl.JLTY OF SCIENCE AND ENGINEERING DEPARTMENT OF PHYSICS
UNIVESITY OF SWAZILAND FACl.LTY OF SCIENCE AND ENGINEERING DEPARTMENT OF PHYSICS Main Examination 2016/2017. COURSE NAME: Thermodynamics/Thermofluids COURSE CODE: PHY242/EEE202 TIME ALLOWED: 3 hours ANSWER
More informationThermal and Statistical Physics Department Exam Last updated November 4, L π
Thermal and Statistical Physics Department Exam Last updated November 4, 013 1. a. Define the chemical potential µ. Show that two systems are in diffusive equilibrium if µ 1 =µ. You may start with F =
More informationChapter 14. The Ideal Gas Law and Kinetic Theory
Chapter 14 The Ideal Gas Law and Kinetic Theory 14.1 Molecular Mass, the Mole, and Avogadro s Number The atomic number of an element is the # of protons in its nucleus. Isotopes of an element have different
More informationThe Kinetic Theory of Gases
PHYS102 Previous Exam Problems CHAPTER 19 The Kinetic Theory of Gases Ideal gas RMS speed Internal energy Isothermal process Isobaric process Isochoric process Adiabatic process General process 1. Figure
More informationUnit 05 Kinetic Theory of Gases
Unit 05 Kinetic Theory of Gases Unit Concepts: A) A bit more about temperature B) Ideal Gas Law C) Molar specific heats D) Using them all Unit 05 Kinetic Theory, Slide 1 Temperature and Velocity Recall:
More informationHence. The second law describes the direction of energy transfer in spontaneous processes
* Heat and Work The first law of thermodynamics states that: Although energy has many forms, the total quantity of energy is constant. When energy disappears in one form, it appears simultaneously in other
More informationTemperature and Thermometers. Temperature is a measure of how hot or cold something is. Most materials expand when heated.
Heat Energy Temperature and Thermometers Temperature is a measure of how hot or cold something is. Most materials expand when heated. Thermometers are instruments designed to measure temperature. In order
More informationHEAT- I Part - A C D A B. Te m p. Heat input
e m p HE- I Part -. solid material is supplied with heat at a constant rate. he temperature of the material is changing with heat input as shown in the graph. Study the graph carefully and answer the following
More informationThermodynamics & Statistical Mechanics SCQF Level 9, U03272, PHY-3-ThermStat. Thursday 24th April, a.m p.m.
College of Science and Engineering School of Physics H T O F E E U D N I I N V E B R U S I R T Y H G Thermodynamics & Statistical Mechanics SCQF Level 9, U03272, PHY-3-ThermStat Thursday 24th April, 2008
More informationPhysics 5D PRACTICE FINAL EXAM Fall 2013
Print your name: Physics 5D PRACTICE FINAL EXAM Fall 2013 Real Exam is Wednesday December 11 Thimann Lecture 3 4:00-7:00 pm Closed book exam two 8.5x11 sheets of notes ok Note: Avogadro s number N A =
More informationChemistry. Lecture 10 Maxwell Relations. NC State University
Chemistry Lecture 10 Maxwell Relations NC State University Thermodynamic state functions expressed in differential form We have seen that the internal energy is conserved and depends on mechanical (dw)
More information1. (10) True or False: A material with an ideal thermal equation of state must have a constant c v.
AME 54531 Intermediate hermodynamics Examination : Prof. J. M. Powers 7 November 018 1. 10) rue or False: A material with an ideal thermal equation of state must have a constant c v. False. Forsuchamaterialc
More informationTable of Contents [ttc]
Table of Contents [ttc] 1. Equilibrium Thermodynamics I: Introduction Thermodynamics overview. [tln2] Preliminary list of state variables. [tln1] Physical constants. [tsl47] Equations of state. [tln78]
More informationThermodynamics. Fill in the blank (1pt)
Fill in the blank (1pt) Thermodynamics 1. The Newton temperature scale is made up of different points 2. When Antonine Lavoisier began his study of combustion, he noticed that metals would in weight upon
More informationOutline. 1. Work. A. First Law of Thermo. 2. Internal Energy. 1. Work continued. Category: Thermodynamics. III. The Laws of Thermodynamics.
ategory: hermodynamics Outline III. he Laws of hermodynamics A. First Law of hermo B. Second Law of hermo (Entropy). Statistical Mechanics D. References Updated: 04jan A. First Law of hermo. Work 4 Stored
More informationFirst major ( 043 ) a) 180 degrees b) 90 degrees c) 135 degrees d) 45 degrees e) 270 degrees
First major ( 043 ) 1) The displacement of a string carrying a traveling sinusoidal wave is given by y(x,t) = y m sin( kx ωt ϕ ). At time t = 0 the point at x = 0 has a displacement of zero and is moving
More informationLecture 25 Goals: Chapter 18 Understand the molecular basis for pressure and the idealgas
Lecture 5 Goals: Chapter 18 Understand the molecular basis for pressure and the idealgas law. redict the molar specific heats of gases and solids. Understand how heat is transferred via molecular collisions
More informationSpeed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution
Temperature ~ Average KE of each particle Particles have different speeds Gas Particles are in constant RANDOM motion Average KE of each particle is: 3/2 kt Pressure is due to momentum transfer Speed Distribution
More informationOCN 623: Thermodynamic Laws & Gibbs Free Energy. or how to predict chemical reactions without doing experiments
OCN 623: Thermodynamic Laws & Gibbs Free Energy or how to predict chemical reactions without doing experiments Definitions Extensive properties Depend on the amount of material e.g. # of moles, mass or
More informationChapter 12. Temperature and Heat. continued
Chapter 12 Temperature and Heat continued 12.3 The Ideal Gas Law THE IDEAL GAS LAW The absolute pressure of an ideal gas is directly proportional to the Kelvin temperature and the number of moles (n) of
More informationPreliminary Examination - Day 2 August 16, 2013
UNL - Department of Physics and Astronomy Preliminary Examination - Day August 16, 13 This test covers the topics of Quantum Mechanics (Topic 1) and Thermodynamics and Statistical Mechanics (Topic ). Each
More information1 Garrod #5.2: Entropy of Substance - Equation of State. 2
Dylan J. emples: Chapter 5 Northwestern University, Statistical Mechanics Classical Mechanics and hermodynamics - Garrod uesday, March 29, 206 Contents Garrod #5.2: Entropy of Substance - Equation of State.
More informationS15--AP Phys Q4--Heat-Thermo Ch13_14_15 PRACTICE
Name: Class: Date: S5--AP Phys Q4--Heat-Thermo Ch3_4_5 PRACTICE Multiple Choice Identify the choice that best completes the statement or answers the question.. Which of the following is a thermodynamic
More information17-1 Ideal Gases. Gases are the easiest state of matter to describe - All ideal gases exhibit similar behavior.
17-1 Ideal Gases Gases are the easiest state of matter to describe - All ideal gases exhibit similar behavior. An ideal gas is one that is thin enough, that the interactions between molecules can be ignored.
More informationThe Second Law of Thermodynamics (Chapter 4)
The Second Law of Thermodynamics (Chapter 4) First Law: Energy of universe is constant: ΔE system = - ΔE surroundings Second Law: New variable, S, entropy. Changes in S, ΔS, tell us which processes made
More informationReversibility. Processes in nature are always irreversible: far from equilibrium
Reversibility Processes in nature are always irreversible: far from equilibrium Reversible process: idealized process infinitely close to thermodynamic equilibrium (quasi-equilibrium) Necessary conditions
More information(i) T, p, N Gibbs free energy G (ii) T, p, µ no thermodynamic potential, since T, p, µ are not independent of each other (iii) S, p, N Enthalpy H
Solutions exam 2 roblem 1 a Which of those quantities defines a thermodynamic potential Why? 2 points i T, p, N Gibbs free energy G ii T, p, µ no thermodynamic potential, since T, p, µ are not independent
More informationPhysics 2: Fluid Mechanics and Thermodynamics
Physics 2: Fluid Mechanics and Thermodynamics Đào Ngọc Hạnh Tâm Office: A1.503, email: dnhtam@hcmiu.edu.vn HCMIU, Vietnam National University Acknowledgment: Most of these slides are supported by Prof.
More informationPY2005: Thermodynamics
ome Multivariate Calculus Y2005: hermodynamics Notes by Chris Blair hese notes cover the enior Freshman course given by Dr. Graham Cross in Michaelmas erm 2007, except for lecture 12 on phase changes.
More informationPhysics 408 Final Exam
Physics 408 Final Exam Name You are graded on your work (with partial credit where it is deserved) so please do not just write down answers with no explanation (or skip important steps)! Please give clear,
More informationFirst Law CML 100, IIT Delhi SS. The total energy of the system. Contribution from translation + rotation + vibrations.
Internal Energy he total energy of the system. Contribution from translation + rotation + vibrations. Equipartition theorem for the translation and rotational degrees of freedom. 1/ k B Work Path function,
More informationS6. (a) State what is meant by an ideal gas...
IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS TSOKOS CHAPTER 3 TEST REVIEW S1. Thermal energy is transferred through the glass windows of a house mainly by A. conduction. B. radiation.
More informationKINETIC THEORY. was the original mean square velocity of the gas. (d) will be different on the top wall and bottom wall of the vessel.
Chapter Thirteen KINETIC THEORY MCQ I 13.1 A cubic vessel (with faces horizontal + vertical) contains an ideal gas at NTP. The vessel is being carried by a rocket which is moving at a speed of 500m s 1
More informationPhysics 202 Homework 5
Physics 202 Homework 5 Apr 29, 2013 1. A nuclear-fueled electric power plant utilizes a so-called boiling water reac- 5.8 C tor. In this type of reactor, nuclear energy causes water under pressure to boil
More informationIdentify the intensive quantities from the following: (a) enthalpy (b) volume (c) refractive index (d) none of these
Q 1. Q 2. Q 3. Q 4. Q 5. Q 6. Q 7. The incorrect option in the following table is: H S Nature of reaction (a) negative positive spontaneous at all temperatures (b) positive negative non-spontaneous regardless
More informationChapter 18 Thermal Properties of Matter
Chapter 18 Thermal Properties of Matter In this section we define the thermodynamic state variables and their relationship to each other, called the equation of state. The system of interest (most of the
More informationS = k log W CHEM Thermodynamics. Change in Entropy, S. Entropy, S. Entropy, S S = S 2 -S 1. Entropy is the measure of dispersal.
, S is the measure of dispersal. The natural spontaneous direction of any process is toward greater dispersal of matter and of energy. Dispersal of matter: Thermodynamics We analyze the constraints on
More informationFirst Law of Thermodynamics
First Law of Thermodynamics E int = Q + W other state variables E int is a state variable, so only depends on condition (P, V, T, ) of system. Therefore, E int only depends on initial and final states
More informationPhysics 2: Fluid Mechanics and Thermodynamics
Physics 2: Fluid Mechanics and Thermodynamics Đào Ngọc Hạnh Tâm Office: A1.503, email: dnhtam@hcmiu.edu.vn HCMIU, Vietnam National University Acknowledgment: Most of these slides are supported by Prof.
More informationCHAPTER 3 TEST REVIEW
IB PHYSICS Name: Period: Date: # Marks: 52 Raw Score: IB Curve: DEVIL PHYSICS BADDEST CLASS ON CAMPUS CHAPTER 3 TEST REVIEW 1. Water at a temperature of 0 C is kept in a thermally insulated container.
More informationPhysics 111. Lecture 42 (Walker: 18.9) Entropy & Disorder Final Review. May 15, 2009
Physics 111 Lecture 42 (Walker: 18.9) Entropy & Disorder Final Review May 15, 2009 Review Session: Today, 3:10-4:00, TH230. Final exam, Monday May 18, 10:45-1:15. Lecture 42 1/32 The Physics 111 Final
More informationCompiled and rearranged by Sajit Chandra Shakya
1 (a) (i) The kinetic theory of gases leads to the equation m = kt. (b) Explain the significance of the quantity m... the equation to suggest what is meant by the absolute zero of temperature...
More informationKinetic theory of the ideal gas
Appendix H Kinetic theory of the ideal gas This Appendix contains sketchy notes, summarizing the main results of elementary kinetic theory. The students who are not familiar with these topics should refer
More informationTB [103 marks] The damping of the system is now increased. Which describes the change in ƒ 0 and the change in A 0?
TB [103 marks] 1. A periodic driving force of frequency ƒ acts on a system which undergoes forced oscillations of amplitude A. The graph below shows the variation with ƒ of A. The maximum amplitude A 0
More informationCYL Classical Thermodynamics Sample Problems
CYL110 2012-2013 Classical Thermodynamics Sample Problems 1. Dieterici s equation of state for a gas is P (V b) exp(a/rv T ) = RT, where a, b, and R are constants. Determine ( V/ T ), ( T/ P ), and ( P/
More informationTHE ZEROTH AND FISRT LAW OF THERMODYNAMICS. Saeda Al-Mhyawi secend Tearm 1435H
H ZROH AND FISR LAW OF HRMODYNAMIS Saeda Al-Mhyawi secend earm 435H HAR II H ZROH AND FISR LAW OF HRMODYNAMIS Lecture () Outline Introduction he Zeroth Law of hermodynamics he First Law of hermodynamics
More information1. Thermodynamics 1.1. A macroscopic view of matter
1. Thermodynamics 1.1. A macroscopic view of matter Intensive: independent of the amount of substance, e.g. temperature,pressure. Extensive: depends on the amount of substance, e.g. internal energy, enthalpy.
More informationPhysics 119A Final Examination
First letter of last name Name: Perm #: Email: Physics 119A Final Examination Thursday 10 December, 2009 Question 1 / 25 Question 2 / 25 Question 3 / 15 Question 4 / 20 Question 5 / 15 BONUS Total / 100
More informationTopic 3 &10 Review Thermodynamics
Name: Date: Topic 3 &10 Review Thermodynamics 1. The kelvin temperature of an object is a measure of A. the total energy of the molecules of the object. B. the total kinetic energy of the molecules of
More informationPhysics 213. Practice Final Exam Spring The next two questions pertain to the following situation:
The next two questions pertain to the following situation: Consider the following two systems: A: three interacting harmonic oscillators with total energy 6ε. B: two interacting harmonic oscillators, with
More informationdv = adx, where a is the active area of the piston. In equilibrium, the external force F is related to pressure P as
Chapter 3 Work, heat and the first law of thermodynamics 3.1 Mechanical work Mechanical work is defined as an energy transfer to the system through the change of an external parameter. Work is the only
More informationChapter 10. Thermal Physics
Chapter 10 Thermal Physics Thermal Physics Thermal physics is the study of Temperature Heat How these affect matter Thermal Physics, cont Descriptions require definitions of temperature, heat and internal
More informationData Provided: A formula sheet and table of physical constants are attached to this paper.
Data Provided: A formula sheet and table of physical constants are attached to this paper. DEPARTMENT OF PHYSICS AND ASTRONOMY Spring Semester (2016-2017) From Thermodynamics to Atomic and Nuclear Physics
More informationFinal Exam for Physics 176. Professor Greenside Wednesday, April 29, 2009
Print your name clearly: Signature: I agree to neither give nor receive aid during this exam Final Exam for Physics 76 Professor Greenside Wednesday, April 29, 2009 This exam is closed book and will last
More information