Q.Consider a rectangular block of wood moving with a velocity v0 in a gas at temperature T and mass density ρ. Assume the velocity is along x-axis and the area of cross-section of the block perpendicular to v0 is A. Show that the drag force on the block is 4ρAv0mkT, where m is the mass of the gas molecule.
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Kinetic Theory Explanation
Imagine you're sitting in a quiet room. The air around you feels still, but it isn't. Every second, billions of tiny particles — molecules of nitrogen and oxygen — are zipping past you at hundreds of metres per second. You don't feel them because they're too small, and they're moving in every direction at once. But if you put your hand near a hot stove, you suddenly feel heat. Why?
The answer is the kinetic theory of matter. It's a way of explaining what we observe at the human scale (temperature, pressure, heat) by thinking about what's happening at the molecular scale.
The core idea
The kinetic theory says three simple things:
- All matter is made of tiny particles (atoms or molecules) that are in constant, random motion.
- The particles collide with each other and with the walls of their container — these collisions are perfectly elastic (no energy is lost).
- The average kinetic energy of these particles is directly proportional to the temperature of the substance.
That's it. Everything else — pressure, diffusion, the way a gas expands when heated — follows from these three statements.
Building intuition
Think of a single gas molecule bouncing around inside a box. It hits a wall, bounces off, and keeps going. Each time it hits the wall, it exerts a tiny force. Now multiply that by billions of molecules hitting every square centimetre of wall every second. That constant, collective force is what we measure as pressure.
Now heat the box. The molecules move faster — their average kinetic energy increases. They hit the walls harder and more often. Pressure goes up. If the walls can move (like a piston), the gas expands until the pressure inside equals the pressure outside.
This is why a bicycle tyre feels hot after you pump it: you're doing work on the air, compressing it, which increases the average kinetic energy of the molecules — and that's exactly what temperature is.
Temperature is not the total kinetic energy of all molecules — it's the average kinetic energy per molecule. A large cold object can have more total energy than a small hot one, but its molecules move slower on average.
The precise statement
For an ideal gas (a gas where intermolecular forces are negligible and collisions are perfectly elastic), the kinetic theory gives us a direct mathematical link:
Average kinetic energy per molecule=23kBT
where kB is Boltzmann's constant (1.38×10−23J/K) and T is the absolute temperature in Kelvin.
This means that at the same temperature, all gas molecules — regardless of their mass — have the same average kinetic energy. A light hydrogen molecule moves faster than a heavy oxygen molecule at the same temperature, but their average kinetic energies are equal.
From this, we can derive the ideal gas law:
PV=31Nmv2=NkBT
where P is pressure, V is volume, N is the number of molecules, m is the mass of one molecule, and v2 is the mean square speed.
PV=nRT
This is the familiar ideal gas law. The kinetic theory shows it's not just an empirical rule — it follows directly from the motion of molecules.
What the theory explains
The kinetic theory isn't just abstract. It explains everyday phenomena:
- Evaporation cools you: The fastest molecules escape from a liquid surface, leaving behind slower ones. The average kinetic energy drops — so the temperature drops.
- Diffusion: Molecules spread out because they're constantly moving and colliding, gradually mixing with neighbouring molecules.
- Brownian motion: Pollen grains jitter under a microscope because they're being bombarded unevenly by invisible water molecules. …
Concept: Kinetic Theory Explanation
Model the gas using the same simplified kinetic-theory picture used to derive gas pressure: treat the molecules as moving only along the three coordinate axes, with n/2 of the molecules moving in the +x direction and n/2 moving in the −x direction (where n=ρ/m is the number density), each with the characteristic 1-D thermal speed vx defined by
21mvx2=21kT⇒vx=mkT.
Step 1 — Collisions on the front face. In the block's rest frame (block moving at v0 along +x), the molecules that were moving in the −x direction (density n/2, speed vx) approach the front face with relative speed (vx+v0). In an elastic collision with the (much heavier) block, each such molecule transfers momentum 2m(vx+v0). The number of such collisions per unit area per unit time is (n/2)(vx+v0), so the pressure on the front face is
Pfront=2n(vx+v0)⋅2m(vx+v0)=nm(vx+v0)2.
Step 2 — Collisions on the back face. Molecules originally moving in the +x direction (density n/2, speed vx) strike the back face with relative speed (vx−v0), transferring momentum 2m(vx−v0) each:
Pback=2n(vx−v0)⋅2m(vx−v0)=nm(vx−v0)2. …
Concept: Kinetic Theory Explanation
Model the gas using the same simplified kinetic-theory picture used to derive gas pressure: treat the molecules as moving only along the three coordinate axes, with n/2 of the molecules moving in the +x direction and n/2 moving in the −x direction (where n=ρ/m is the number density), each with the characteristic 1-D thermal speed vx defined by
21mvx2=21kT⇒vx=mkT.
Step 1 — Collisions on the front face. In the block's rest frame (block moving at v0 along +x), the molecules that were moving in the −x direction (density n/2, speed vx) approach the front face with relative speed (vx+v0). In an elastic collision with the (much heavier) block, each such molecule transfers momentum 2m(vx+v0). The number of such collisions per unit area per unit time is (n/2)(vx+v0), so the pressure on the front face is
Pfront=2n(vx+v0)⋅2m(vx+v0)=nm(vx+v0)2.
Step 2 — Collisions on the back face. Molecules originally moving in the +x direction (density n/2, speed vx) strike the back face with relative speed (vx−v0), transferring momentum 2m(vx−v0) each:
Pback=2n(vx−v0)⋅2m(vx−v0)=nm(vx−v0)2. …
Alternate approach — dimensional analysis pins down the formula's shape. The only quantities available to build a drag force from are ρ, A, v0, and the thermal speed scale kT/m (the sole velocity that k, T, m can combine into). A force has units of kg⋅m/s2, and ρAv0kT/m already carries exactly those units (density × area × velocity × velocity), so any correct expression for the drag in this regime must be proportional to ρAv0kT/m — the full momentum-transfer calculation i …
- AP EAPCET 2022Set ap-2022-07-12-FN1 markMCQQ.Principles of molecular interactions and thermal energy can be used to explain (I) Vapour Pressure (II) Surface Tension (III) Viscosity (A) (I) and (II) only (B) (II) and (III) only (C) (I) and (III) only (D) (I), (II) and (III)
›Reveal solutionSolution
All three phenomena — vapour pressure, surface tension, and viscosity — arise from the competition between intermolecular attractive forces and the thermal kinetic energy of molecules. Answer: all three, (D).
Concept and Intuition
Molecules in a liquid are held together by intermolecular attractive forces, but they also possess thermal kinetic energy that lets them move and, at the surface, occasionally escape. Vapour pressure is set by how many molecules have enough thermal energy to overcome the attractive pull and evaporate. Surface tension arises because surface molecules feel a net inward pull from their neighbours (fewer neighbours above), an effect governed by the strength of intermolecular forces relative to thermal jostling. Viscosity reflects the internal friction between layers of a fluid sliding past each other, which again depends on how strongly molecules interact and how much thermal energy resists that ordered interaction.
Step-by-Step Solution
- Vapour pressure: molecules escape the liquid surface once their thermal KE exceeds the attractive potential holding them in — directly a molecular-interaction/thermal-energy balance.
- Surface tension: surface molecules experience net inward intermolecular attraction (asymmetric neighbour distribution), which is why it depends on both the interaction strength and temperature (thermal agitation reduces it). …
- AP EAPCET 2022Set eng-2022-07-06-AN1 markMCQQ.Assertion (A) : When an ideal gas is compressed adiabatically its temperature and the average kinetic energy of the gas molecules increase. Reason (R) : The kinetic energy increases because of collisions of molecules with moving parts of wall only. (A) (A) and (R) are true and (R) is correct explanation of (A) (B) (A) and (R) are true but (R) is not correct explanation of (A) (C) (A) is true and (R) is false (D) (A) is false and (R) is true
›Reveal solutionSolution
Both statements are true, and the moving-wall-collision mechanism in the Reason is indeed the correct microscopic explanation for why adiabatic compression raises the gas's temperature.
Concept and Intuition
Thermodynamically, adiabatic compression means Q=0, so all the work done ON the gas goes into raising its internal energy (and hence temperature, for an ideal gas). Kinetic theory gives the microscopic picture: a gas molecule that elastically collides with a wall moving toward it (as the piston advances) rebounds with a higher speed than it had — exactly like a ball gaining speed when struck by an approaching bat/paddle. Collisions with a stationary wall, by contrast, are perfectly elastic in the sense that the molecule's speed (in the wall's frame) doesn't change. So it is precisely the collisions with the moving piston that pump kinetic energy into the gas.
Step-by-Step Solution
- Assertion: during adiabatic compression, Q=0 and work is done on the gas, so ΔU=−Wbygas>0 (since Wbygas<0 for compression). For an ideal gas, U∝T, so T rises, and since average KE per molecule ∝T, the average KE also rises. Assertion is true. …
- AP EAPCET 2021Set ap-2021-09-03-FN1 markMCQQ.In the kinetic theory of gases, it is assumed that the gas molecules: (A) Repel each other (B) Collide elastically (C) Move with uniform velocity (D) Are massless particles
›Reveal solutionSolution
One of the founding postulates of kinetic theory is that molecular collisions are perfectly elastic, conserving kinetic energy.
Concept and Intuition
Kinetic theory models a gas as a huge number of tiny, hard particles in random motion. For the theory's predictions (like the ideal gas law and Maxwell speed distribution) to hold, the total kinetic energy of the gas must be conserved during collisions — otherwise the gas would spontaneously cool or heat as molecules collided, which isn't observed for an isolated ideal gas. Hence molecule–molecule and molecule–wall collisions are assumed perfectly elastic.
Step-by-Step Solution
- Kinetic theory postulates: molecules are point particles (negligible size compared to separation), in continuous random motion, exerting no force on each other except during collisions, and collisions (with each other and the container walls) are perfectly elastic.
- "Repel each other" is not a general assumption — intermolecular forces are neglected except at contact. …
- AP EAPCET 2021Set eng-2021-10-05-FN1 markMCQQ.Temperature determines the direction of net change of ___________ (A) gross Kinetic energy (B) gross Potential energy (C) intermolecular Potential energy (D) intermolecular Kinetic energy
›Reveal solutionSolution
Temperature reflects the average kinetic energy of random molecular motion; it is this intermolecular kinetic energy whose net exchange between bodies (heat flow) is dictated by temperature difference.
Concept and Intuition
Microscopically, temperature is a measure of the average kinetic energy of the disordered, random motion of molecules (translational, and to some extent rotational/vibrational) — not any ordered, bulk ('gross') motion of the object as a whole, and not the potential energy stored in intermolecular bonds/configuration. When two bodies at different temperatures are placed in contact, energy flows (as heat) in the direction that equalizes this molecular kinetic energy, always from the hotter (higher average molecular KE) to the colder body, until thermal equilibrium is reached. This is precisely the microscopic content of the zeroth and second laws: temperature — not total internal energy or potential energy — determines the direction of net thermal energy transfer.
Step-by-Step Solution
- Recognize that gross (bulk) kinetic/potential energy refers to a body's overall, macroscopic mechanical energy (e.g. a moving block), which is unrelated to temperature.
- Recognize that intermolecular potential energy relates to bonding/configuration between molecules (relevant to phase changes, not to the direction of heat flow between two bodies at different temperatures). …
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