Complete Solutions and Summary of Thermodynamics – NCERT Class 11, Physics, Chapter 11 – Summary, Questions, Answers, Extra Questions
Summary of thermal equilibrium, Zeroth law, heat, internal energy and work, first and second laws of thermodynamics, specific heat capacities, thermodynamic processes, Carnot engine, and solved NCERT problems.
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Thermodynamics
Chapter 11: Physics - Ultimate Study Guide | NCERT Class 11 Notes, Questions, Examples & Quiz 2025
Full Chapter Summary & Detailed Notes - Thermodynamics Class 11 NCERT
Overview & Key Concepts
- Chapter Goal: Introduces thermodynamics as the study of heat, work, and energy interconversions in macroscopic systems, without molecular details. Covers laws governing thermal energy, equilibrium, processes, and efficiency. Exam Focus: Zeroth/First/Second Laws, specific heats, processes (isothermal/adiabatic), Carnot cycle calculations. 2025 Updates: Reprint emphasizes historical context (Rumford experiment), real-world apps like engines/refrigerators; tables on specific heats. Fun Fact: Thermodynamics predates kinetic theory; Carnot (1824) laid heat engine foundations. Core Idea: Energy conservation (First Law) but directionality (Second Law) limits efficiency. Real-World: Steam engines, ACs, climate change (entropy increase). Ties: Builds on Ch.10 thermal properties; leads to Ch.12 kinetic theory.
- Wider Scope: Foundation for engineering (power plants), environmental science (heat engines in climate models), astrophysics (stellar engines).
11.1 Introduction
Thermodynamics studies heat-temperature interconversions and energy forms, focusing on bulk systems (macroscopic variables like P, V, T). Unlike microscopic kinetic theory (molecular velocities), it uses few measurable variables. Distinction from mechanics: Mechanics concerns ordered motion (KE of body); thermo internal disordered energy (temperature-related). Historical: Caloric fluid theory discarded post-Rumford (1798) cannon boring experiment—heat from work, not fluid. Depth: Rubbing palms (work→heat); steam engine (heat→work). Questions: Why heat flows hot→cold? Directionality key. Real-Life: Internal combustion engines convert chemical heat to mechanical work. Exam Tip: Macro vs micro; no molecular details. Extended: Zeroth Law defines temperature; First conserves energy; Second entropy. Links: Ch.9 fluids (P-V); Ch.12 gases (PV=nRT). Graphs: No visuals, but conceptual caloric flow analogy (water levels equalize).
- Examples: Bullet stops (KE→heat); insulated gas equilibrium (no change in P,V,T).
- Point: Thermodynamics 19th century, pre-molecular theory.
Extended Discussion: Scope: Reversible processes ideal; irreversible real (friction). Pitfalls: Heat not state variable (transit energy). Applications: Power cycles (Rankine). Depth: Units: Heat J (SI); calorie obsolete. Interlinks: Biology (metabolic heat). Advanced: Statistical mechanics bridges macro-micro. Real: Solar panels (photovoltaic, but thermo limits efficiency). Historical: Sadi Carnot father of thermo. NCERT: Focus energy conversion; Rumford key experiment. Principles: Laws empirical from observations. Errors: Confuse heat (Q) with U (internal). Scope: Closed/open systems.
Principles: Macroscopic, equilibrium states. Advanced: Non-equilibrium thermo (Prigogine). Vector: No, scalar variables. Applications: HVAC systems. Common: Ignore path dependence of Q,W.
11.2 Thermal Equilibrium
Equilibrium: Macro variables (P,V,T,m,composition) constant over time. Depends on surroundings/walls: Adiabatic (insulating, no heat flow, Fig.11.1a: A,B independent); Diathermic (conducting, heat flows till T equal, Fig.11.1b: Equilibrium when no net flow). Depth: For gases, independent variables P,V (or T,V). Real-Life: Thermos (adiabatic walls). Exam Tip: Equilibrium if isolated/insulated; thermal when T same. Extended: Quasi-static slow changes. Ties: Zeroth Law basis. Graphs: Fig.11.1 walls; no P-V yet.
- Examples: Closed rigid insulated gas (equilibrium); two gases diathermic (T equalize, P,V adjust).
- SI: Variables measurable (senses).
Extended: Phase equilibrium (Ch.5). Pitfalls: Mechanical equilibrium (F=0) vs thermal. Applications: Calorimeters (diathermic contact). Depth: Extensive (V,m) vs intensive (P,T). Interlinks: Ch.13 oscillations (damped to equilibrium). Advanced: Local equilibrium approximation. Real: Room thermostat (equilibrium seek). Historical: Clausius equilibrium. NCERT: Walls define interaction; gases P,V independent.
Principles: No change in time. Errors: Equilibrium absolute? Relative to surroundings. Scope: Bulk systems.
11.3 Zeroth Law of Thermodynamics
If A,B thermal equilibrium with C separately (Fig.11.2a: conducting to C, adiabatic between), then A,B equilibrium when connected (Fig.11.2b). Defines temperature T: Equal T implies equilibrium. Formulated by Fowler (1931) post First/Second Laws. Depth: Transitive property; T scale construction (thermometry). Real-Life: Thermometer (C as reference). Exam Tip: Zeroth because foundational; T same for equilibrium. Extended: Absolute scale Kelvin. Ties: Thermal equilibrium section. Graphs: Fig.11.2 setups.
- Examples: Two bodies via third (T_A = T_C = T_B).
- Limitations: Assumes no other interactions.
Extended Discussion: Atomic: T ∝ average KE. Pitfalls: T not just hotness (negative K possible). Applications: IR thermography. Depth: Scales: Celsius (water), Kelvin (absolute). Interlinks: Ch.10 expansion (T scale). Advanced: Negative T spin systems. Real: Weather stations. Historical: Ranked zeroth retrospectively. NCERT: Clue to T concept.
Principles: Empirical; enables T measurement. Errors: Assume ideal contacts.
11.4 Heat, Internal Energy and Work
Heat Q: Energy transit due to ΔT (Fig.11.4a: flow hot→cold). Internal U: Sum molecular KE+PE (disordered, CM rest frame, Fig.11.3: excludes bulk motion). Work W: Energy transfer non-ΔT (Fig.11.4b: piston push). Depth: U state variable (path independent); Q,W path dependent (not states). Real-Life: Rubbing (W→U); engine (Q→W). Exam Tip: Q not stored; U depends on state (P,V,T). Extended: For ideal gas U=f(T) only. Ties: First Law. Graphs: Fig.11.3 molecular motions; Fig.11.4 modes.
- Examples: Gas cylinder: Heat raises T (Q→U); compress (W→U).
- State variables: P,V,T,U (macro).
Extended: Molecular: Translational/rotational/vibrational (Ch.12). Pitfalls: "Gas has heat" meaningless. Applications: Calorimetry (Q measure). Depth: U extensive; T intensive. Interlinks: Ch.6 work-energy. Advanced: Enthalpy H=U+PV. Real: Batteries (chemical U→electrical W). Historical: Joule equivalence. NCERT: Distinguish Q (transit) vs U (state).
Principles: Two modes change U: Q,W. Errors: U includes only random motion.
11.5 First Law of Thermodynamics
ΔQ = ΔU + ΔW (conservation; Q supplied = U increase + work by system). For constant P: ΔW=PΔV, ΔQ=ΔU + PΔV. Path independent: ΔU; path dependent: Q,W. Depth: Cyclic ΔU=0, ∮Q=∮W. Real-Life: Isothermal expansion ideal gas ΔU=0, Q=W. Exam Tip: Sign: ΔW by system positive. Extended: Applications: Water vaporization ΔU=2087J (most to U, little PΔV). Ties: Eq.11.3. Graphs: No, but P-V work area.
- Examples: 1g water latent 2256J, ΔW=169J, ΔU=2087J.
- Alternative: ΔU=ΔQ - ΔW.
Extended Discussion: Joule's experiment verifies. Pitfalls: Signs convention (IUPAC: W on system negative). Applications: Refrigerators (Q extract, W input). Depth: Open systems mass flow. Interlinks: Ch.3 Kinematics (work). Advanced: Enthalpy for constant P ΔH=ΔQ. Real: IC engines cycles. Historical: Clausius 1850. NCERT: General energy conservation.
Principles: No creation/destruction. Errors: Assume closed system.
11.6 Specific Heat Capacity
Heat capacity S=ΔQ/ΔT; specific s=S/m (J/kg K); molar C=S/μ (J/mol K). For solids ~3R (Dulong-Petit, equipartition 3D oscillator). Depth: Water s=4186 J/kg K; varies T (Fig.11.5). For gases: C_p - C_v = R (ideal, Eq.11.8 proof: C_v=ΔU/ΔT, C_p=C_v + R). Real-Life: Water high s (climate moderation). Exam Tip: Calorie=4.186J (14.5-15.5°C). Extended: C_v= (f/2)R (f degrees freedom). Ties: Table 11.1 solids ~3R. Graphs: Fig.11.5 water curve.
- Examples: Solids C=3R=25 J/mol K; carbon exception low T.
- Gases: Constant V (ΔU), P (ΔH).
Extended: Low T quantum (Debye). Pitfalls: s independent mass? No, per kg. Applications: Calorimeters. Depth: Polyatomic f=6, C_v=3R. Interlinks: Ch.12 kinetic. Advanced: C_p/C_v=γ adiabatic. Real: Cooking (water s). Historical: Dulong-Petit 1819. NCERT: Predicts solids; gases relation.
Principles: ΔQ=m s ΔT. Errors: Ignore process (V/P).
11.7 Thermodynamic State Variables and Equation of State
Equilibrium specified by state variables (P,V,T,U,S extensive/intensive). Equation of state: Relates (e.g., PV=μRT ideal gas). Depth: Not always equilibrium (free expansion Fig.11.6a rapid). Real-Life: P-V-T gauges. Exam Tip: 2 independent for gas (P,V fix T). Extended: Van der Waals real gas. Ties: Processes. Graphs: Fig.11.6 non-equilibrium.
- Examples: Gas state (P1,V1) to (P2,V2) path varies Q,W but ΔU fixed.
- Five variables: P,V,T,U,S.
Extended: Phase rule. Pitfalls: All variables independent? No. Applications: Compressors. Depth: Intensive unchanged subsystems. Interlinks: Ch.5 ideal gas. Advanced: Entropy S state. Real: Weather models. Historical: Boyle-Charles. NCERT: Macro description.
Principles: Complete specification. Errors: Free expansion ΔU=0 but not quasi-static.
11.8 Thermodynamic Processes
Quasi-static: Slow, equilibrium at each step. Types: Isothermal (ΔT=0, ΔU=0 ideal, Q=W); Adiabatic (Q=0, ΔU=-W); Isobaric (ΔP=0, W=PΔV); Isochoric (ΔV=0, W=0); Cyclic (back to start, ∮dU=0). Depth: P-V diagrams (area=W). Real-Life: Refrigerator cycle. Exam Tip: Adiabatic no heat exchange. Extended: Polytropic PV^n. Ties: Second Law. Graphs: P-V paths.
- Examples: Isothermal expansion Q=μRT ln(V2/V1).
- Reversible: Quasi-static + no dissipation.
Extended: Efficiency calculations. Pitfalls: All processes quasi-static? No. Applications: Otto cycle. Depth: Work ∫PdV. Interlinks: Ch.3 graphs. Advanced: T-S diagrams. Real: Breathing (isobaric?). Historical: Clausius processes. NCERT: Path defines Q,W.
Principles: Change from state i to f. Errors: Cyclic Q net ≠0.
11.9 Second Law of Thermodynamics
Heat cannot flow cold→hot without work (Kelvin); cannot convert heat fully to work without temp difference (Clausius). Entropy ΔS=ΔQ_rev/T increases isolated (ΔS≥0). Depth: Directionality; efficiency <1. Real-Life: Engines η=1-T_c/T_h. Exam Tip: Irreversibility entropy rise. Extended: Statistical (Boltzmann S=k lnΩ). Ties: Carnot. Graphs: No.
- Examples: Ice melts (ΔS>0); heat engine rejects Q_c.
- Absolute: No perpetual motion II.
Extended: Universe entropy increases (heat death). Pitfalls: First conserves, Second directs. Applications: Refrigerators COP. Depth: Reversible ΔS=0. Interlinks: Ch.12 disorder. Advanced: Black hole entropy. Real: Greenhouse (trapped heat). Historical: Clausius 1850. NCERT: Kelvin-Planck/Clausius statements.
Principles: Asymmetry time. Errors: Assume reversible always.
11.10 Reversible and Irreversible Processes
Reversible: Quasi-static, no friction, ΔS=0 (ideal); Irreversible: Real, finite speed, ΔS>0 (e.g., free expansion). Depth: All real irreversible. Real-Life: Slow compression reversible approx. Exam Tip: Reversible for max work. Extended: Hysteresis. Ties: Second Law. Graphs: No.
- Examples: Adiabatic free expansion irreversible (ΔU=0, W=0, Q=0 but ΔS>0).
- Criteria: Undo without change surroundings.
Extended: Onsager reciprocity. Pitfalls: Quasi-static always reversible? No if dissipative. Applications: Max efficiency reversible. Depth: ΔS_universe=ΔS_sys + ΔS_surr. Interlinks: Ch.14 damping. Advanced: Non-equilibrium. Real: Diffusion irreversible. Historical: Carathéodory 1909. NCERT: Basis Carnot.
Principles: Ideal vs real. Errors: Ignore friction.
11.11 Carnot Engine
Ideal reversible cycle: Isothermal expansion (Q_h absorb), adiabatic expansion, isothermal compression (Q_c reject), adiabatic compression. Efficiency η=1 - T_c/T_h (independent working substance). Depth: Max possible; all reversible same η. Real-Life: Benchmark Otto/Diesel. Exam Tip: T Kelvin. Extended: Carnot theorem. Ties: Second Law. Graphs: P-V rectangle-like.
- Examples: T_h=600K, T_c=300K, η=50%.
- Refrigerator: COP= T_c/(T_h - T_c).
Extended: Multi-stage. Pitfalls: Real < Carnot. Applications: Power plants. Depth: W=Q_h - Q_c. Interlinks: Ch.12 ideal gas. Advanced: Ericsson cycle. Real: Stirling approx Carnot. Historical: Sadi Carnot 1824. NCERT: Highest efficiency.
Principles: Reversible cycle limit. Errors: Absolute T.
Summary
- Thermo macro; equilibrium constant variables; Zeroth T equal; U state, Q/W path; First ΔQ=ΔU+ΔW; s=ΔQ/mΔT, C_p-C_v=R; States P,V,T; Processes quasi-static; Second ΔS≥0; Reversible ideal; Carnot η=1-T_c/T_h.
Why This Guide Stands Out
Complete: All subtopics (11+), examples solved (water vapor), Q&A exam-style, 30 numericals. Physics-focused with eqs/graphs/tables. Free for 2025.
Key Themes & Tips
- Laws: 0th defines T, 1st conserves, 2nd directs.
- Processes: Isothermal ΔU=0, adiabatic Q=0.
- Tip: Memorize signs; practice P-V work; units J.
Exam Case Studies
Vaporization ΔU calc; Carnot η.
Project & Group Ideas
- Model heat engine: Stirling, measure η.
- P-V diagram: App simulate processes.
Group Discussions
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