Kinetic Theory PDF

CHAPTER THIRTEEN KINETIC THEORY 13.1 INTRODUCTION Boyle discovered the law named after him in 1661. Boyle,...

CHAPTER THIRTEEN KINETIC THEORY 13.1 INTRODUCTION Boyle discovered the law named after him in 1661. Boyle, Newton and several others tried to explain the behaviour of 13.1 Introduction gases by considering that gases are made up of tiny atomic 13.2 Molecular nature of matter particles. The actual atomic theory got established more than 13.3 Behaviour of gases 150 years later. Kinetic theory explains the behaviour of gases 13.4 Kinetic theory of an ideal gas based on the idea that the gas consists of rapidly moving 13.5 Law of equipartition of energy atoms or molecules. This is possible as the inter-atomic forces, 13.6 Specific heat capacity which are short range forces that are important for solids 13.7 Mean free path and liquids, can be neglected for gases. The kinetic theory was developed in the nineteenth century by Maxwell, Summary Boltzmann and others. It has been remarkably successful. It Points to ponder gives a molecular interpretation of pressure and temperature Exercises of a gas, and is consistent with gas laws and Avogadro’s Additional exercises hypothesis. It correctly explains specific heat capacities of many gases. It also relates measurable properties of gases such as viscosity, conduction and diffusion with molecular parameters, yielding estimates of molecular sizes and masses. This chapter gives an introduction to kinetic theory. 13.2 MOLECULAR NATURE OF MATTER Richard Feynman, one of the great physicists of 20th century considers the discovery that “Matter is made up of atoms” to be a very significant one. Humanity may suffer annihilation (due to nuclear catastrophe) or extinction (due to environmental disasters) if we do not act wisely. If that happens, and all of scientific knowledge were to be destroyed then Feynman would like the ‘Atomic Hypothesis’ to be communicated to the next generation of creatures in the universe. Atomic Hypothesis: All things are made of atoms - little particles that move around in perpetual motion, attracting each other when they are a little distance apart, but repelling upon being squeezed into one another. Speculation that matter may not be continuous, existed in many places and cultures. Kanada in India and Democritus 2022-23 324 PHYSICS Atomic Hypothesis in Ancient India and Greece Though John Dalton is credited with the introduction of atomic viewpoint in modern science, scholars in ancient India and Greece conjectured long before the existence of atoms and molecules. In the Vaiseshika school of thought in India founded by Kanada (Sixth century B.C.) the atomic picture was developed in considerable detail. Atoms were thought to be eternal, indivisible, infinitesimal and ultimate parts of matter. It was argued that if matter could be subdivided without an end, there would be no difference between a mustard seed and the Meru mountain. The four kinds of atoms (Paramanu — Sanskrit word for the smallest particle) postulated were Bhoomi (Earth), Ap (water), Tejas (fire) and Vayu (air) that have characteristic mass and other attributes, were propounded. Akasa (space) was thought to have no atomic structure and was continuous and inert. Atoms combine to form different molecules (e.g. two atoms combine to form a diatomic molecule dvyanuka, three atoms form a tryanuka or a triatomic molecule), their properties depending upon the nature and ratio of the constituent atoms. The size of the atoms was also estimated, by conjecture or by methods that are not known to us. The estimates vary. In Lalitavistara, a famous biography of the Buddha written mainly in the second century B.C., the estimate is close to the modern estimate of atomic size, of the order of 10 –10 m. In ancient Greece, Democritus (Fourth century B.C.) is best known for his atomic hypothesis. The word ‘atom’ means ‘indivisible’ in Greek. According to him, atoms differ from each other physically, in shape, size and other properties and this resulted in the different properties of the substances formed by their combination. The atoms of water were smooth and round and unable to ‘hook’ on to each other, which is why liquid /water flows easily. The atoms of earth were rough and jagged, so they held together to form hard substances. The atoms of fire were thorny which is why it caused painful burns. These fascinating ideas, despite their ingenuity, could not evolve much further, perhaps because they were intuitive conjectures and speculations not tested and modified by quantitative experiments - the hallmark of modern science. in Greece had suggested that matter may consist of matter. The theory is now well accepted by of indivisible constituents. The scientific ‘Atomic scientists. However even at the end of the Theory’ is usually credited to John Dalton. He nineteenth century there were famous scientists proposed the atomic theory to explain the laws who did not believe in atomic theory ! of definite and multiple proportions obeyed by From many observations, in recent times we elements when they combine into compounds. now know that molecules (made up of one or The first law says that any given compound has, more atoms) constitute matter. Electron a fixed proportion by mass of its constituents. microscopes and scanning tunnelling The second law says that when two elements microscopes enable us to even see them. The form more than one compound, for a fixed mass size of an atom is about an angstrom (10 -10 m). of one element, the masses of the other elements In solids, which are tightly packed, atoms are are in ratio of small integers. spaced about a few angstroms (2 Å) apart. In To explain the laws Dalton suggested, about liquids the separation between atoms is also 200 years ago, that the smallest constituents about the same. In liquids the atoms are not of an element are atoms. Atoms of one element as rigidly fixed as in solids, and can move are identical but differ from those of other around. This enables a liquid to flow. In gases elements. A small number of atoms of each the interatomic distances are in tens of element combine to form a molecule of the angstroms. The average distance a molecule compound. Gay Lussac’s law, also given in early can travel without colliding is called the mean 19th century, states: When gases combine free path. The mean free path, in gases, is of chemically to yield another gas, their volumes the order of thousands of angstroms. The atoms are in the ratios of small integers. Avogadro’s are much freer in gases and can travel long law (or hypothesis) says: Equal volumes of all distances without colliding. If they are not gases at equal temperature and pressure have enclosed, gases disperse away. In solids and the same number of molecules. Avogadro’s law, liquids the closeness makes the interatomic force when combined with Dalton’s theory explains important. The force has a long range attraction Gay Lussac’s law. Since the elements are often and a short range repulsion. The atoms attract in the form of molecules, Dalton’s atomic theory when they are at a few angstroms but repel when can also be referred to as the molecular theory they come closer. The static appearance of a gas 2022-23 KINETIC THEORY 325 is misleading. The gas is full of activity and the for a given sample of the gas. Here T is the equilibrium is a dynamic one. In dynamic temperature in kelvin or (absolute) scale. K is a equilibrium, molecules collide and change their constant for the given sample but varies with speeds during the collision. Only the average the volume of the gas. If we now bring in the properties are constant. idea of atoms or molecules, then K is proportional Atomic theory is not the end of our quest, but to the number of molecules, (say) N in the the beginning. We now know that atoms are not sample. We can write K = N k. Observation tells indivisible or elementary. They consist of a us that this k is same for all gases. It is called nucleus and electrons. The nucleus itself is made Boltzmann constant and is denoted by k. B up of protons and neutrons. The protons and P1V1 PV neutrons are again made up of quarks. Even As = 2 2 = constant = kB (13.2) N1T1 N 2 T2 quarks may not be the end of the story. There may be string like elementary entities. Nature if P, V and T are same, then N is also same for always has surprises for us, but the search for all gases. This is Avogadro’s hypothesis, that the truth is often enjoyable and the discoveries number of molecules per unit volume is beautiful. In this chapter, we shall limit ourselves the same for all gases at a fixed temperature and to understanding the behaviour of gases (and a pressure. The number in 22.4 litres of any gas little bit of solids), as a collection of moving is 6.02 × 1023. This is known as Avogadro molecules in incessant motion. number and is denoted by NA. The mass of 22.4 litres of any gas is equal to its molecular weight 13.3 BEHAVIOUR OF GASES in grams at S.T.P (standard temperature 273 K Properties of gases are easier to understand than and pressure 1 atm). This amount of substance those of solids and liquids. This is mainly is called a mole (see Chapter 2 for a more precise because in a gas, molecules are far from each definition). Avogadro had guessed the equality of other and their mutual interactions are numbers in equal volumes of gas at a fixed negligible except when two molecules collide. temperature and pressure from chemical Gases at low pressures and high temperatures reactions. Kinetic theory justifies this hypothesis. much above that at which they liquefy (or The perfect gas equation can be written as solidify) approximately satisfy a simple relation PV = µ RT (13.3) between their pressure, temperature and volume where µ is the number of moles and R = NA given by (see Chapter 11) kB is a universal constant. The temperature T is PV = KT (13.1) absolute temperature. Choosing kelvin scale for John Dalton (1766 – 1844) He was an English chemist. When different types of atoms combine, they obey certain simple laws. Dalton’s atomic theory explains these laws in a simple way. He also gave a theory of colour blindness. Amedeo Avogadro (1776 – 1856) He made a brilliant guess that equal volumes of gases have equal number of molecules at the same temperature and pressure. This helped in understanding the combination of different gases in a very simple way. It is now called Avogadro’s hypothesis (or law). He also suggested that the smallest constituent of gases like hydrogen, oxygen and nitrogen are not atoms but diatomic molecules. 2022-23 326 PHYSICS absolute temperature, R = 8.314 J mol–1K–1. i.e., keeping temperature constant, pressure of Here a given mass of gas varies inversely with volume. This is the famous Boyle’s law. Fig. 13.2 shows M N µ = = (13.4) comparison between experimental P-V curves M0 NA and the theoretical curves predicted by Boyle’s where M is the mass of the gas containing N law. Once again you see that the agreement is molecules, M0 is the molar mass and NA the good at high temperatures and low pressures. Avogadro’s number. Using Eqs. (13.4) and (13.3) Next, if you fix P, Eq. (13.1) shows that V ∝ T can also be written as i.e., for a fixed pressure, the volume of a gas is PV = kB NT or P = kB nT proportional to its absolute temperature T (Charles’ law). See Fig. 13.3. ( J mol –1K –1) pV µT P (atm) Fig.13.1 Real gases approach ideal gas behaviour at low pressures and high temperatures. where n is the number density, i.e. number of molecules per unit volume. kB is the Boltzmann Fig.13.2 Experimental P-V curves (solid lines) for constant introduced above. Its value in SI units steam at three temperatures compared is 1.38 × 10–23 J K–1. with Boyle’s law (dotted lines). P is in units Another useful form of Eq. (13.3) is of 22 atm and V in units of 0.09 litres. ρRT P = (13.5) Finally, consider a mixture of non-interacting M0 ideal gases: µ moles of gas 1, µ moles of gas where ρ is the mass density of the gas. 1 2 2, etc. in a vessel of volume V at temperature T A gas that satisfies Eq. (13.3) exactly at all and pressure P. It is then found that the pressures and temperatures is defined to be an equation of state of the mixture is : ideal gas. An ideal gas is a simple theoretical model of a gas. No real gas is truly ideal. PV = ( µ1 + µ2 +… ) RT (13.7) Fig. 13.1 shows departures from ideal gas RT RT behaviour for a real gas at three different i.e. P = µ1 + µ2 +... (13.8) temperatures. Notice that all curves approach V V the ideal gas behaviour for low pressures and = P1 + P2 + … (13.9) high temperatures. Clearly P1 = µ1 R T/V is the pressure that At low pressures or high temperatures the gas 1 would exert at the same conditions of molecules are far apart and molecular volume and temperature if no other gases were interactions are negligible. Without interactions present. This is called the partial pressure of the the gas behaves like an ideal one. gas. Thus, the total pressure of a mixture of ideal If we fix µ and T in Eq. (13.3), we get gases is the sum of partial pressures. This is PV = constant (13.6) Dalton’s law of partial pressures. 2022-23 KINETIC THEORY 327 density of water molecule may therefore, be regarded as roughly equal to the density of bulk water = 1000 kg m–3. To estimate the volume of a water molecule, we need to know the mass of a single water molecule. We know that 1 mole of water has a mass approximately equal to (2 + 16)g = 18 g = 0.018 kg. Since 1 mole contains about 6 × 1023 molecules (Avogadro’s number), the mass of a molecule of water is (0.018)/(6 × 1023) kg = 3 × 10–26 kg. Therefore, a rough estimate of the volume of a water molecule is as follows : Volume of a water molecule = (3 × 10–26 kg)/ (1000 kg m–3) = 3 × 10–29 m3 = (4/3) π (Radius)3 Fig. 13.3 Experimental T-V curves (solid lines) for Hence, Radius ≈ 2 ×10-10 m = 2 Å t CO2 at three pressures compared with Charles’ law (dotted lines). T is in units of What is the average t Example 13.3 300 K and V in units of 0.13 litres. distance between atoms (interatomic distance) in water? Use the data given in We next consider some examples which give Examples 13.1 and 13.2. us information about the volume occupied by the molecules and the volume of a single Answer : A given mass of water in vapour state molecule. has 1.67×103 times the volume of the same mass of water in liquid state (Ex. 13.1). This is also Example 13.1 The density of water is 1000 t the increase in the amount of volume available kg m–3. The density of water vapour at 100 °C for each molecule of water. When volume and 1 atm pressure is 0.6 kg m–3. The increases by 103 times the radius increases by volume of a molecule multiplied by the total V1/3 or 10 times, i.e., 10 × 2 Å = 20 Å. So the number gives ,what is called, molecular average distance is 2 × 20 = 40 Å. t volume. Estimate the ratio (or fraction) of the molecular volume to the total volume Example 13.4 A vessel contains two non- t occupied by the water vapour under the reactive gases : neon (monatomic) and above conditions of temperature and oxygen (diatomic). The ratio of their partial pressure. pressures is 3:2. Estimate the ratio of (i) number of molecules and (ii) mass density Answer For a given mass of water molecules, of neon and oxygen in the vessel. Atomic the density is less if volume is large. So the mass of Ne = 20.2 u, molecular mass of O2 volume of the vapour is 1000/0.6 = 1/(6 ×10 -4 ) = 32.0 u. times larger. If densities of bulk water and water molecules are same, then the fraction of Answer Partial pressure of a gas in a mixture is molecular volume to the total volume in liquid the pressure it would have for the same volume state is 1. As volume in vapour state has and temperature if it alone occupied the vessel. increased, the fractional volume is less by the (The total pressure of a mixture of non-reactive same amount, i.e. 6×10-4. t gases is the sum of partial pressures due to its constituent gases.) Each gas (assumed ideal) Example 13.2 Estimate the volume of a t obeys the gas law. Since V and T are common to water molecule using the data in Example the two gases, we have P1V = µ 1 RT and P2V = 13.1. µ2 RT, i.e. (P1/P2) = (µ1 / µ2). Here 1 and 2 refer Answer In the liquid (or solid) phase, the to neon and oxygen respectively. Since (P1/P2) = molecules of water are quite closely packed. The (3/2) (given), (µ1/ µ2) = 3/2. 2022-23 328 PHYSICS (i) By definition µ1 = (N1/NA ) and µ2 = (N2/NA) where N1 and N2 are the number of molecules of 1 and 2, and NA is the Avogadro’s number. Therefore, (N1/N2) = (µ1 / µ2) = 3/2. (ii) We can also write µ1 = (m1/M1) and µ2 = (m2/M2) where m1 and m2 are the masses of 1 and 2; and M1 and M2 are their molecular masses. (Both m1 and M1; as well as m2 and M2 should be expressed in the same units). If ρ1 and ρ2 are the mass densities of 1 and 2 respectively, we have ρ1 m /V m µ M  = 1 = 1 = 1 × 1 Fig. 13.4 Elastic collision of a gas molecule with ρ2 m2 /V m 2 µ2  M 2  the wall of the container. 3 20.2 (vx, vy, vz ) hits the planar wall parallel to yz- = × = 0.947 t 2 32.0 plane of area A (= l 2). Since the collision is elastic, the molecule rebounds with the same velocity; 13.4 KINETIC THEORY OF AN IDEAL GAS its y and z components of velocity do not change in the collision but the x-component reverses Kinetic theory of gases is based on the molecular sign. That is, the velocity after collision is picture of matter. A given amount of gas is a (-vx, vy, vz ). The change in momentum of the collection of a large number of molecules molecule is: –mvx – (mvx) = – 2mvx. By the (typically of the order of Avogadro’s number) that principle of conservation of momentum, the are in incessant random motion. At ordinary momentum imparted to the wall in the collision pressure and temperature, the average distance = 2mvx. between molecules is a factor of 10 or more than To calculate the force (and pressure) on the the typical size of a molecule (2 Å). Thus, wall, we need to calculate momentum imparted interaction between molecules is negligible and to the wall per unit time. In a small time interval we can assume that they move freely in straight ∆t, a molecule with x-component of velocity vx lines according to Newton’s first law. However, will hit the wall if it is within the distance vx ∆t occasionally, they come close to each other, from the wall. That is, all molecules within the experience intermolecular forces and their volume Avx ∆t only can hit the wall in time ∆t. velocities change. These interactions are called But, on the average, half of these are moving collisions. The molecules collide incessantly towards the wall and the other half away from against each other or with the walls and change the wall. Thus, the number of molecules with their velocities. The collisions are considered to velocity (vx, vy, vz ) hitting the wall in time ∆t is be elastic. We can derive an expression for the ½A vx ∆t n, where n is the number of molecules pressure of a gas based on the kinetic theory. per unit volume. The total momentum We begin with the idea that molecules of a gas are in incessant random motion, colliding transferred to the wall by these molecules in against one another and with the walls of the time ∆t is : container. All collisions between molecules Q = (2mvx) (½ n A vx ∆t ) (13.10) among themselves or between molecules and the The force on the wall is the rate of momentum walls are elastic. This implies that total kinetic transfer Q/∆t and pressure is force per unit energy is conserved. The total momentum is area : conserved as usual. P = Q /(A ∆t) = n m vx2 (3.11) Actually, all molecules in a gas do not have 13.4.1 Pressure of an Ideal Gas the same velocity; there is a distribution in velocities. The above equation, therefore, stands Consider a gas enclosed in a cube of side l. Take for pressure due to the group of molecules with the axes to be parallel to the sides of the cube, speed vx in the x-direction and n stands for the as shown in Fig. 13.4. A molecule with velocity number density of that group of molecules. The 2022-23 KINETIC THEORY 329 total pressure is obtained by summing over the the gas in equilibrium is the same as anywhere contribution due to all groups: else. Second, we have ignored any collisions in P = n m v x2 (13.12) the derivation. Though this assumption is difficult to justify rigorously, we can qualitatively where v x is the average of vx. Now the gas 2 2 see that it will not lead to erroneous results. is isotropic, i.e. there is no preferred direction The number of molecules hitting the wall in time of velocity of the molecules in the vessel. ∆t was found to be ½ n Avx ∆t. Now the collisions Therefore, by symmetry, are random and the gas is in a steady state. 2 Thus, if a molecule with velocity (vx, vy, vz ) v 2x = vy = v z2 acquires a different velocity due to collision with = (1/3) [ v 2x + v y2 + v z2 ] = (1/3) v 2 (13.13) some molecule, there will always be some other molecule with a different initial velocity which where v is the speed and v 2 denotes the mean after a collision acquires the velocity (vx, vy, vz ). If this were not so, the distribution of velocities of the squared speed. Thus would not remain steady. In any case we are P = (1/3) n m v 2 (13.14) finding v x2. Thus, on the whole, molecular Some remarks on this derivation. First, collisions (if they are not too frequent and the though we choose the container to be a cube, time spent in a collision is negligible compared the shape of the vessel really is immaterial. For to time between collisions) will not affect the a vessel of arbitrary shape, we can always choose calculation above. a small infinitesimal (planar) area and carry 13.4.2 Kinetic Interpretation of Temperature through the steps above. Notice that both A and ∆t do not appear in the final result. By Pascal’s Equation (13.14) can be written as law, given in Ch. 10, pressure in one portion of PV = (1/3) nV m v 2 (13.15a) Founders of Kinetic Theory of Gases James Clerk Maxwell (1831 – 1879), born in Edinburgh, Scotland, was among the greatest physicists of the nineteenth century. He derived the thermal velocity distribution of molecules in a gas and was among the first to obtain reliable estimates of molecular parameters from measurable quantities like viscosity, etc. Maxwell’s greatest achievement was the unification of the laws of electricity and magnetism (discovered by Coulomb, Oersted, Ampere and Faraday) into a consistent set of equations now called Maxwell’s equations. From these he arrived at the most important conclusion that light is an electromagnetic wave. Interestingly, Maxwell did not agree with the idea (strongly suggested by the Faraday’s laws of electrolysis) that electricity was particulate in nature. Ludwig Boltzmann (1844 – 1906) bor n in Vienna, Austria, worked on the kinetic theory of gases independently of Maxwell. A firm advocate of atomism, that is basic to kinetic theory, Boltzmann provided a statistical interpretation of the Second Law of thermodynamics and the concept of entropy. He is regarded as one of the founders of classical statistical mechanics. The proportionality constant connecting energy and temperature in kinetic theory is known as Boltzmann’s constant in his honour. 2022-23 330 PHYSICS PV = (2/3) N x ½ m v 2 (13.15b) M N2 28 where N (= nV ) is the number of molecules in m = = = 4.65 × 10 –26 kg. NA 6.02 × 1026 the sample. The quantity in the bracket is the average v 2 = 3 kB T / m = (516)2 m2s-2 translational kinetic energy of the molecules in The square root of v 2 is known as root mean the gas. Since the internal energy E of an ideal square (rms) speed and is denoted by vrms, gas is purely kinetic*, ( We can also write v 2 as < v2 >.) E = N × (1/2) m v 2 (13.16) vrms = 516 m s-1 Equation (13.15) then gives : The speed is of the order of the speed of sound PV = (2/3) E (13.17) in air. It follows from Eq. (13.19) that at the same We are now ready for a kinetic interpretation temperature, lighter molecules have greater rms of temperature. Combining Eq. (13.17) with the speed. ideal gas Eq. (13.3), we get t Example 13.5 A flask contains argon and E = (3/2) kB NT (13.18) chlorine in the ratio of 2:1 by mass. The or E/ N = ½ m v 2 = (3/2) kBT (13.19) temperature of the mixture is 27 °C. Obtain i.e., the average kinetic energy of a molecule is the ratio of (i) average kinetic energy per proportional to the absolute temperature of the molecule, and (ii) root mean square speed gas; it is independent of pressure, volume or vrms of the molecules of the two gases. the nature of the ideal gas. This is a fundamental Atomic mass of argon = 39.9 u; Molecular result relating temperature, a macroscopic mass of chlorine = 70.9 u. measurable parameter of a gas (a thermodynamic variable as it is called) to a Answer The important point to remember is that molecular quantity, namely the average kinetic the average kinetic energy (per molecule) of any energy of a molecule. The two domains are (ideal) gas (be it monatomic like argon, diatomic connected by the Boltzmann constant. We note in passing that Eq. (13.18) tells us that internal like chlorine or polyatomic) is always equal to energy of an ideal gas depends only on (3/2) kBT. It depends only on temperature, and temperature, not on pressure or volume. With is independent of the nature of the gas. this interpretation of temperature, kinetic theory (i) Since argon and chlorine both have the same of an ideal gas is completely consistent with the temperature in the flask, the ratio of average ideal gas equation and the various gas laws kinetic energy (per molecule) of the two gases based on it. is 1:1. For a mixture of non-reactive ideal gases, the (ii) Now ½ m vrms2 = average kinetic energy per total pressure gets contribution from each gas molecule = (3/2) ) kBT where m is the mass in the mixture. Equation (13.14) becomes of a molecule of the gas. Therefore, P = (1/3) [n1m1 v12 + n2 m2 v 22 +… ] (13.20) In equilibrium, the average kinetic energy of (v ) 2 rms Ar = (m )Cl = (M )Cl 70.9 the molecules of different gases will be equal. That is, (v ) 2 rms Cl (m )Ar ( M ) Ar = 39.9 =1.77 where M denotes the molecular mass of the gas. ½ m1 v12 = ½ m2 v 22 = (3/2) kB T (For argon, a molecule is just an atom of argon.) so that Taking square root of both sides, P = (n1 + n2 +… ) kB T (13.21) which is Dalton’s law of partial pressures. (v ) rms Ar From Eq. (13.19), we can get an idea of the (v ) rms Cl = 1.33 typical speed of molecules in a gas. At a temperature T = 300 K, the mean square speed You should note that the composition of the of a molecule in nitrogen gas is : mixture by mass is quite irrelevant to the above * E denotes the translational part of the internal energy U that may include energies due to other degrees of freedom also. See section 13.5. 2022-23 KINETIC THEORY 331 Maxwell Distribution Function In a given mass of gas, the velocities of all molecules are not the same, even when bulk parameters like pressure, volume and temperature are fixed. Collisions change the direction and the speed of molecules. However in a state of equilibrium, the distribution of speeds is constant or fixed. Distributions are very important and useful when dealing with systems containing large number of objects. As an example consider the ages of different persons in a city. It is not feasible to deal with the age of each individual. We can divide the people into groups: children up to age 20 years, adults between ages of 20 and 60, old people above 60. If we want more detailed information we can choose smaller intervals, 0-1, 1-2,..., 99-100 of age groups. When the size of the interval becomes smaller, say half year, the number of persons in the interval will also reduce, roughly half the original number in the one year interval. The number of persons dN(x) in the age interval x and x+dx is proportional to dx or dN(x) = nx dx. We have used nx to denote the number of persons at the value of x. Maxwell distribution of molecular speeds In a similar way the molecular speed distribution gives the number of molecules between 2 the speeds v and v+ dv. dN(v) = 4p N a3e–bv v2 dv = nvdv. This is called Maxwell distribution. The plot of nv against v is shown in the figure. The fraction of the molecules with speeds v and v+dv is equal to the area of the strip shown. The average of any quantity like v2 is defined by the integral = (1/N ) ∫ v2 dN(v) = ª(3kB T/m) which agrees with the result derived from more elementary considerations. mass of the molecule, faster will be the speed. calculation. Any other proportion by mass of The ratio of speeds is inversely proportional to argon and chlorine would give the same answers the square root of the ratio of the masses. The to (i) and (ii), provided the temperature remains masses are 349 and 352 units. So unaltered. t v349 / v352 = ( 352/ 349)1/2 = 1.0044. Example 13.6 Uranium has two isotopes t ∆V of masses 235 and 238 units. If both are Hence difference = 0.44 %. present in Uranium hexafluoride gas which V would have the larger average speed ? If [235U is the isotope needed for nuclear fission. atomic mass of fluorine is 19 units, To separate it from the more abundant isotope estimate the percentage difference in 238 U, the mixture is surrounded by a porous speeds at any temperature. cylinder. The porous cylinder must be thick and narrow, so that the molecule wanders through Answer At a fixed temperature the average individually, colliding with the walls of the long energy = ½ m is constant. So smaller the pore. The faster molecule will leak out more than 2022-23 332 PHYSICS the slower one and so there is more of the lighter is V + u towards the bat. When the ball rebounds molecule (enrichment) outside the porous (after hitting the massive bat) its speed, relative cylinder (Fig. 13.5). The method is not very to bat, is V + u moving away from the bat. So efficient and has to be repeated several times relative to the wicket the speed of the rebounding for sufficient enrichment.]. t ball is V + (V + u) = 2V + u, moving away from When gases diffuse, their rate of diffusion is the wicket. So the ball speeds up after the inversely proportional to square root of the collision with the bat. The rebound speed will masses (see Exercise 13.12 ). Can you guess the be less than u if the bat is not massive. For a explanation from the above answer? molecule this would imply an increase in temperature. You should be able to answer (b) (c) and (d) based on the answer to (a). (Hint: Note the correspondence, pistonà bat, cylinder à wicket, molecule à ball.) t 13.5 LAW OF EQUIPARTITION OF ENERGY The kinetic energy of a single molecule is 1 1 1 εt = mv x2 + mvy2 + mv z2 (13.22) 2 2 2 For a gas in ther mal equilibrium at temperature T the average value of energy denoted by < ε t > is 1 1 1 3 εt = mv x2 + mvy2 + mv z2 = k B T (13.23) 2 2 2 2 Fig. 13.5 Molecules going through a porous wall. Since there is no preferred direction, Eq. (13.23) Example 13.7 (a) When a molecule (or implies t an elastic ball) hits a ( massive) wall, it 1 1 1 1 rebounds with the same speed. When a ball mv x2 = kBT , mv y2 = kBT , 2 2 2 2 hits a massive bat held firmly, the same thing happens. However, when the bat is 1 1 moving towards the ball, the ball rebounds mv z2 = kBT (13.24) 2 2 with a different speed. Does the ball move faster or slower? (Ch.6 will refresh your A molecule free to move in space needs three memory on elastic collisions.) coordinates to specify its location. If it is constrained to move in a plane it needs two; and (b) When gas in a cylinder is compressed if constrained to move along a line, it needs just by pushing in a piston, its temperature one coordinate to locate it. This can also be rises. Guess at an explanation of this in expressed in another way. We say that it has terms of kinetic theory using (a) above. one degree of freedom for motion in a line, two (c) What happens when a compressed gas for motion in a plane and three for motion in pushes a piston out and expands. What space. Motion of a body as a whole from one would you observe ? point to another is called translation. Thus, a (d) Sachin Tendulkar used a heavy cricket molecule free to move in space has three bat while playing. Did it help him in translational degrees of freedom. Each anyway ? translational degree of freedom contributes a term that contains square of some variable of Answer (a) Let the speed of the ball be u relative motion, e.g., ½ mvx2 and similar terms in to the wicket behind the bat. If the bat is moving vy and vz. In, Eq. (13.24) we see that in thermal towards the ball with a speed V relative to the equilibrium, the average of each such term is wicket, then the relative speed of the ball to bat ½ kBT. 2022-23 KINETIC THEORY 333 Molecules of a monatomic gas like argon have ε = εt + εr + εv (13.26) only translational degrees of freedom. But what where k is the force constant of the oscillator about a diatomic gas such as O2 or N 2? A and y the vibrational co-ordinate. molecule of O2 has three translational degrees Once again the vibrational energy terms in of freedom. But in addition it can also rotate Eq. (13.26) contain squared terms of vibrational about its centre of mass. Figure 13.6 shows the variables of motion y and dy/dt. two independent axes of rotation 1 and 2, normal At this point, notice an important feature in to the axis joining the two oxygen atoms about which the molecule can rotate*. The molecule Eq.(13.26). While each translational and thus has two rotational degrees of freedom, each rotational degree of freedom has contributed only of which contributes a term to the total energy one ‘squared term’ in Eq.(13.26), one vibrational consisting of translational energy εt and mode contributes two ‘squared terms’ : kinetic rotational energy ε r. and potential energies. Each quadratic term occurring in the 1 1 1 1 1 εt + εr = mv x2 + mvy2 + mv z2 + I1ω12 + I 2 ω 22 (13.25) expression for energy is a mode of absorption of 2 2 2 2 2 energy by the molecule. We have seen that in thermal equilibrium at absolute temperature T, for each translational mode of motion, the average energy is ½ kBT. The most elegant principle of classical statistical mechanics (first proved by Maxwell) states that this is so for each mode of energy: translational, rotational and vibrational. That is, in equilibrium, the total energy is equally distributed in all possible energy modes, with each mode having an average energy equal to ½ kBT. This is known as the law of equipartition of energy. Accordingly, each Fig. 13.6 The two independent axes of rotation of a translational and rotational degree of freedom diatomic molecule of a molecule contributes ½ kBT to the energy, while each vibrational frequency contributes where ω1 and ω2 are the angular speeds about 2 × ½ kBT = kBT , since a vibrational mode has the axes 1 and 2 and I1, I2 are the corresponding both kinetic and potential energy modes. moments of inertia. Note that each rotational The proof of the law of equipartition of energy degree of freedom contributes a term to the is beyond the scope of this book. Here, we shall energy that contains square of a rotational apply the law to predict the specific heats of variable of motion. gases theoretically. Later, we shall also discuss We have assumed above that the O2 molecule briefly, the application to specific heat of solids. is a ‘rigid rotator’, i.e., the molecule does not vibrate. This assumption, though found to be true (at moderate temperatures) for O2, is not 13.6 SPECIFIC HEAT CAPACITY always valid. Molecules, like CO, even at 13.6.1 Monatomic Gases moderate temperatures have a mode of vibration, i.e., its atoms oscillate along the interatomic axis The molecule of a monatomic gas has only three like a one-dimensional oscillator, and contribute translational degrees of freedom. Thus, the a vibrational energy term εv to the total energy: average energy of a molecule at temperature T is (3/2)kBT. The total internal energy of a mole 2 1  dy  1 2 of such a gas is εv = m  + ky 2  dt 2 * Rotation along the line joining the atoms has very small moment of inertia and does not come into play for quantum mechanical reasons. See end of section 13.6. 2022-23 334 PHYSICS i.e.,Cv = (3 + f ) R, Cp = (4 + f ) R, 3 3 U = k B T × N A = RT (13.27) 2 2 (4 + f ) γ = (13.36) (3 + f ) The molar specific heat at constant volume, Cv, is Note that Cp – Cv = R is true for any ideal gas, whether mono, di or polyatomic. dU 3 Cv (monatomic gas) = = RT (13.28) Table 13.1 summarises the theoretical dT 2 predictions for specific heats of gases ignoring For an ideal gas, any vibrational modes of motion. The values are Cp – Cv = R (13.29) in good agreement with experimental values of where Cp is the molar specific heat at constant specific heats of several gases given in Table 13.2. pressure. Thus, Of course, there are discrepancies between 5 predicted and actual values of specific heats of Cp = R (13.30) several other gases (not shown in the table), such 2 as Cl2, C2H6 and many other polyatomic gases. Cp 5 Usually, the experimental values for specific The ratio of specific heats γ = = (13.31) Cv 3 heats of these gases are greater than the predicted values as given in Table13.1 suggesting 13.6.2 Diatomic Gases that the agreement can be improved by including vibrational modes of motion in the calculation. As explained earlier, a diatomic molecule treated The law of equipartition of energy is, thus, well as a rigid rotator, like a dumbbell, has 5 degrees of freedom: 3 translational and 2 rotational. Using the law of equipartition of energy, the total Table 13.1 Predicted values of specific heat internal energy of a mole of such a gas is capacities of gases (ignoring 5 5 vibrational modes) U = kBT × N A = RT (13.32) 2 2 Nature of Cv Cp Cp - Cv The molar specific heats are then given by g Gas 1 1 1 1 1 1 (J mol- K- ) (J mol- K- ) (J mol- K- ) 5 7 Cv (rigid diatomic) = R, Cp = R (13.33) Monatomic 12.5 20.8 8.31 1.67 2 2 Diatomic 20.8 29.1 8.31 1.40 7 γ (rigid diatomic) = (13.34) Triatomic 24.93 33.24 8.31 1.33 5 If the diatomic molecule is not rigid but has in addition a vibrational mode Table13.2 Measured values of specific heat 5  7 capacities of some gases U =  k BT + k B T  N A = RT  2  2 7 9 9 Cv = R, C p = R, γ = R (13.35) 2 2 7 13.6.3 Polyatomic Gases In general a polyatomic molecule has 3 translational, 3 rotational degrees of freedom and a certain number ( f ) of vibrational modes. According to the law of equipartition of energy, it is easily seen that one mole of such a gas has 3 U =  kBT + 3 kBT + f kBT NA 2 2 2022-23 KINETIC THEORY 335 verified experimentally at ordinary As Table 13.3 shows the prediction generally temperatures. agrees with experimental values at ordinary temperature (Carbon is an exception). Example 13.8 A cylinder of fixed capacity t 44.8 litres contains helium gas at standard 13.6.5 Specific Heat Capacity of Water temperature and pressure. What is the amount of heat needed to raise the We treat water like a solid. For each atom average temperature of the gas in the cylinder by energy is 3kBT. Water molecule has three atoms, 15.0 °C ? (R = 8.31 J mo1–1 K–1). two hydrogen and one oxygen. So it has Answer Using the gas law PV = µRT, you can U = 3 × 3 kBT × NA = 9 RT easily show that 1 mol of any (ideal) gas at and C = ∆Q/ ∆T =∆ U / ∆T = 9R. standard temperature (273 K) and pressure This is the value observed and the agreement (1 atm = 1.01 × 105 Pa) occupies a volume of 22.4 litres. This universal volume is called molar is very good. In the calorie, gram, degree units, volume. Thus the cylinder in this example water is defined to have unit specific heat. As 1 contains 2 mol of helium. Further, since helium calorie = 4.179 joules and one mole of water is monatomic, its predicted (and observed) molar is 18 grams, the heat capacity per mole is specific heat at constant volume, Cv = (3/2) R, ~ 75 J mol-1 K-1 ~ 9R. However with more and molar specific heat at constant pressure, complex molecules like alcohol or acetone the Cp = (3/2) R + R = (5/2) R. Since the volume of arguments, based on degrees of freedom, become the cylinder is fixed, the heat required is more complicated. determined by Cv. Therefore, Lastly, we should note an important aspect Heat required = no. of moles × molar specific of the predictions of specific heats, based on the heat × rise in temperature classical law of equipartition of energy. The = 2 × 1.5 R × 15.0 = 45 R predicted specific heats are independent of = 45 × 8.31 = 374 J. t temperature. As we go to low temperatures, however, there is a marked departure from this 13.6.4 Specific Heat Capacity of Solids prediction. Specific heats of all substances We can use the law of equipartition of energy to approach zero as T à0. This is related to the determine specific heats of solids. Consider a fact that degrees of freedom get frozen and solid of N atoms, each vibrating about its mean ineffective at low temperatures. According to position. An oscillation in one dimension has classical physics, degrees of freedom must average energy of 2 × ½ kBT = kBT. In three remain unchanged at all times. The behaviour dimensions, the average energy is 3 kBT. For a of specific heats at low temperatures shows the mole of solid, N = N A , and the total inadequacy of classical physics and can be energy is explained only by invoking quantum U = 3 kBT × NA = 3 RT considerations, as was first shown by Einstein. Now at constant pressure ∆Q = ∆U + P∆V Quantum mechanics requires a minimum, = ∆U, since for a solid ∆V is negligible. Hence, non-zero amount of energy before a degree of ∆Q ∆U freedom comes into play. This is also the reason C = = = 3R (13.37) ∆T ∆T why vibrational degrees of freedom come into play Table 13.3 Specific Heat Capacity of some only in some cases. solids at room temperature and atmospheric pressure 13.7 MEAN FREE PATH Molecules in a gas have rather large speeds of the order of the speed of sound. Yet a gas leaking from a cylinder in a kitchen takes considerable time to diffuse to the other corners of the room. The top of a cloud of smoke holds together for hours. This happens because molecules in a gas have a finite though small size, so they are bound to undergo collisions. As a result, they cannot 2022-23 336 PHYSICS Seeing is Believing Can one see atoms rushing about. Almost but not quite. One can see pollen grains of a flower being pushed around by molecules of water. The size of the grain is ~ 10-5 m. In 1827, a Scottish botanist Robert Brown, while examining, under a microscope, pollen grains of a flower suspended in water noticed that they continuously moved about in a zigzag, random fashion. Kinetic theory provides a simple explanation of the phenomenon. Any object suspended in water is continuously bombarded from all sides by the water molecules. Since the motion of molecules is random, the number of molecules hitting the object in any direction is about the same as the number hitting in the opposite direction. The small difference between these molecular hits is negligible compared to the total number of hits for an object of ordinary size, and we do not notice any movement of the object. When the object is sufficiently small but still visible under a microscope, the difference in molecular hits from different directions is not altogether negligible, i.e. the impulses and the torques given to the suspended object through continuous bombardment by the molecules of the medium (water or some other fluid) do not exactly sum to zero. There is a net impulse and torque in this or that direction. The suspended object thus, moves about in a zigzag manner and tumbles about randomly. This motion called now ‘Brownian motion’ is a visible proof of molecular activity. In the last 50 years or so molecules have been seen by scanning tunneling and other special microscopes. In 1987 Ahmed Zewail, an Egyptian scientist working in USA was able to observe not only the molecules but also their detailed interactions. He did this by illuminating them with flashes of laser light for very short durations, of the order of tens of femtoseconds and photographing them. ( 1 femto- second = 10-15 s ). One could study even the formation and breaking of chemical bonds. That is really seeing ! move straight unhindered; their paths keep will collide with it (see Fig. 13.7). If n is the getting incessantly deflected. number of molecules per unit volume, the molecule suffers nπd2 ∆t collisions in time ∆t. Thus the rate of collisions is nπd2 or the time between two successive collisions is on the average, τ = 1/(nπ d2 ) (13.38) The average distance between two successive collisions, called the mean free path l, is : t v l = τ = 1/(nπd2) (13.39) d In this derivation, we imagined the other molecules to be at rest. But actually all molecules are moving and the collision rate is determined d by the average relative velocity of the molecules. Thus we need to replace by in Eq. r (13.38). A more exact treatment gives l = 1/ ( 2 nπ d 2 ) (13.40) Let us estimate l and τ for air molecules with Fig. 13.7 The volume swept by a molecule in time ∆t average speeds = ( 485m/s). At STP in which any molecule will collide with it. (0.02 × 10 ) 23 Suppose the molecules of a gas are spheres n= of diameter d. Focus on a single molecule with (22.4 × 10 ) –3 the average speed. It will suffer collision with = 2.7 × 10 25 m -3. any molecule that comes within a distance d Taking, d = 2 × 10–10 m, between the centres. In time ∆t, it sweeps a τ = 6.1 × 10–10 s volume πd2 ∆t wherein any other molecule and l = 2.9 × 10–7 m ≈ 1500d (13.41) 2022-23 KINETIC THEORY 337 As expected, the mean free path given by 25 273 Eq. (13.40) depends inversely on the number So n = 2.7 × 10 × = 2 × 1025 m –3 density and the size of the molecules. In a highly 373 evacuated tube n is rather small and the mean Hence, mean free path l = 4 × 10 –7 m t free path can be as large as the length of the Note that the mean free path is 100 times the tube. interatomic distance ~ 40 Å = 4 ×10-9 m calculated earlier. It is this large value of mean free path that Example 13.9 Estimate the mean free path t leads to the typical gaseous behaviour. Gases can for a water molecule in water vapour at 373 K. not be confined without a container. Use information from Exercises 13.1 and Using, the kinetic theory of gases, the bulk Eq. (13.41) above. measurable properties like viscosity, heat conductivity and diffusion can be related to the Answer The d for water vapour is same as that microscopic parameters like molecular size. It of air. The number density is inversely is through such relations that the molecular proportional to absolute temperature. sizes were first estimated. SUMMARY 1. The ideal gas equation connecting pressure (P ), volume (V ) and absolute temperature (T ) is PV = µ RT = kB NT where µ is the number of moles and N is the number of molecules. R and kB are universal constants. R R = 8.314 J mol–1 K–1, kB = = 1.38 × 10–23 J K–1 NA Real gases satisfy the ideal gas equation only approximately, more so at low pressures and high temperatures. 2. Kinetic theory of an ideal gas gives the relation 1 P= n m v2 3 where n is number density of molecules, m the mass of the molecule and v 2 is the mean of squared speed. Combined with the ideal gas equation it yields a kinetic interpretation of temperature. 1 3 ( ) 3k B T 1/ 2 m v 2 = k B T , vrms = v 2 = 2 2 m This tells us that the temperature of a gas is a measure of the average kinetic energy of a molecule, independent of the nature of the gas or molecule. In a mixture of gases at a fixed temperature the heavier molecule has the lower average speed. 3. The translational kinetic energy E= 3 kB NT. 2 This leads to a relation 2 PV = E 3 4. The law of equipartition of energy states that if a system is in equilibrium at absolute temperature T, the total energy is distributed equally in different energy modes of 2022-23 338 PHYSICS absorption, the energy in each mode being equal to ½ kB T. Each translational and rotational degree of freedom corresponds to one energy mode of absorption and has energy ½ kB T. Each vibrational frequency has two modes of energy (kinetic and potential) with corresponding energy equal to 2 × ½ kB T = kB T. 5. Using the law of equipartition of energy, the molar specific heats of gases can be determined and the values are in agreement with the experimental values of specific heats of several gases. The agreement can be improved by including vibrational modes of motion. 6. The mean free path l is the average distance covered by a molecule between two successive collisions : 1 l= 2 n π d2 where n is the number density and d the diameter of the molecule. POINTS TO PONDER 1. Pressure of a fluid is not only exerted on the wall. Pressure exists everywhere in a fluid. Any layer of gas inside the volume of a container is in equilibrium because the pressure is the same on both sides of the layer. 2. We should not have an exaggerated idea of the intermolecular distance in a gas. At ordinary pressures and temperatures, this is only 10 times or so the interatomic distance in solids and liquids. What is different is the mean free path which in a gas is 100 times the interatomic distance and 1000 times the size of the molecule. 3. The law of equipartition of energy is stated thus: the energy for each degree of freedom in thermal equilibrium is ½ k T. Each quadratic term in the total energy expression of B a molecule is to be counted as a degree of freedom. Thus, each vibrational mode gives 2 (not 1) degrees of freedom (kinetic and potential energy modes), corresponding to the energy 2 × ½ k T = k T. B B 4. Molecules of air in a room do not all fall and settle on the ground (due to gravity) because of their high speeds and incessant collisions. In equilibrium, there is a very slight increase in density at lower heights (like in the atmosphere). The effect is small since the potential energy (mgh) for ordinary heights is much less than the average kinetic energy ½ mv2 of the molecules. 5. < v2 > is not always equal to ( < v >)2. The average of a squared quantity is not necessarily the square of the average. Can you find examples for this statement. EXERCISES 13.1 Estimate the fraction of molecular volume to the actual volume occupied by oxygen gas at STP. Take the diameter of an oxygen molecule to be 3 Å. 13.2 Molar volume is the volume occupied by 1 mol of any (ideal) gas at standard temperature and pressure (STP : 1 atmospheric pressure, 0 °C). Show that it is 22.4 litres. 13.3 Figure 13.8 shows plot of PV/T versus P for 1.00×10–3 kg of oxygen gas at two different temperatures. 2022-23 KINETIC THEORY 339 y T1 PV (J K–1) T2 T P x Fig. 13.8 (a) What does the dotted plot signify? (b) Which is true: T1 > T2 or T1 < T2? (c) What is the value of PV/T where the curves meet on the y-axis? (d) If we obtained similar plots for 1.00×10–3 kg of hydrogen, would we get the same value of PV/T at the point where the curves meet on the y-axis? If not, what mass of hydrogen yields the same value of PV/T (for low pressure high temperature region of the plot) ? (Molecular mass of H 2 = 2.02 u, of O 2 = 32.0 u, R = 8.31 J mo1–1 K–1.) 13.4 An oxygen cylinder of volume 30 litres has an initial gauge pressure of 15 atm and a temperature of 27 °C. After some oxygen is withdrawn from the cylinder, the gauge pressure drops to 11 atm and its temperature drops to 17 °C. Estimate the mass of oxygen taken out of the cylinder (R = 8.31 J mol–1 K–1, molecular mass of O2 = 32 u). 13.5 An air bubble of volume 1.0 cm3 rises from the bottom of a lake 40 m deep at a temperature of 12 °C. To what volume does it grow when it reaches the surface, which is at a temperature of 35 °C ? 13.6 Estimate the total number of air molecules (inclusive of oxygen, nitrogen, water vapour and other constituents) in a room of capacity 25.0 m3 at a temperature of 27 °C and 1 atm pressure. 13.7 Estimate the average thermal energy of a helium atom at (i) room temperature (27 °C), (ii) the temperature on the surface of the Sun (6000 K), (iii) the temperature of 10 million kelvin (the typical core temperature in the case of a star). 13.8 Three vessels of equal capacity have gases at the same temperature and pressure. The first vessel contains neon (monatomic), the second contains chlorine (diatomic), and the third contains uranium hexafluoride (polyatomic). Do the vessels contain equal number of respective molecules ? Is the root mean square speed of molecules the same in the three cases? If not, in which case is vrms the largest ? 13.9 At what temperature is the root mean square speed of an atom in an argon gas cylinder equal to the rms speed of a helium gas atom at – 20 °C ? (atomic mass of Ar = 39.9 u, of He = 4.0 u). 13.10 Estimate the mean free path and collision frequency of a nitrogen molecule in a cylinder containing nitrogen at 2.0 atm and temperature 17 0C. Take the radius of a nitrogen molecule to be roughly 1.0 Å. Compare the collision time with the time the molecule moves freely between two successive collisions (Molecular mass of N2 = 28.0 u). 2022-23 340 PHYSICS Additional Exercises 13.11 A metre long narrow bore held horizontally (and closed at one end) contains a 76 cm long mercury thread, which traps a 15 cm column of air. What happens if the tube is held vertically with the open end at the bottom ? 13.12 From a certain apparatus, the diffusion rate of hydrogen has an average value of 28.7 cm3 s–1. The diffusion of another gas under the same conditions is measured to have an average rate of 7.2 cm3 s–1. Identify the gas. [Hint : Use Graham’s law of diffusion: R1/R2 = ( M2 /M1 )1/2, where R1, R2 are diffusion rates of gases 1 and 2, and M1 and M2 their respective molecular masses. The law is a simple consequence of kinetic theory.] 13.13 A gas in equilibrium has uniform density and pressure throughout its volume. This is strictly true only if there are no external influences. A gas column under gravity, for example, does not have uniform density (and pressure). As you might expect, its density decreases with height. The precise dependence is given by the so-called law of atmospheres n2 = n1 exp [ -mg (h2 – h1)/ kBT ] where n2, n1 refer to number density at heights h2 and h1 respectively. Use this relation to derive the equation for sedimentation equilibrium of a suspension in a liquid column: n2 = n1 exp [ -mg NA (ρ - ρ′ ) (h2 –h1)/ (ρ RT)] where ρ is the density of the suspended particle, and ρ′ , that of surrounding medium. [NA is Avogadro’s number, and R the universal gas constant.] [Hint : Use Archimedes principle to find the apparent weight of the suspended particle.] 13.14 Given below are densities of some solids and liquids. Give rough estimates of the size of their atoms : Substance Atomic Mass (u) Density (103 Kg m-3) Carbon (diamond) 12.01 2.22 Gold 197.00 19.32 Nitrogen (liquid) 14.01 1.00 Lithium 6.94 0.53 Fluorine (liquid) 19.00 1.14 [Hint : Assume the atoms to be ‘tightly packed’ in a solid or liquid phase, and use the known value of Avogadro’s number. You should, however, not take the actual numbers you obtain for various atomic sizes too literally. Because of the crudeness of the tight packing approximation, the results only indicate that atomic sizes are in the range of a few Å]. 2022-23