1.7.23 · Physics › Thermodynamics
Entropy ek state function hai, lekin irreversibility ke wajah se entropy ka production nahi hoti. Kisi bhi real (irreversible) process mein, system + surroundings ki total entropy badhti hai: Δ S univ > 0 . Reversible processes woh idealized boundary hain jahan Δ S univ = 0 . Koi bhi spontaneous process Δ S univ < 0 ke saath nahi hoti — woh direction hai jo hum nature mein kabhi nahi dekhte.
Definition Entropy (Clausius)
Reversible path ke liye, entropy change ko is tarah define kiya jaata hai:
d S ≡ T δ Q rev
jahan T woh absolute temperature hai jis par heat δ Q rev boundary cross karti hai. Kyunki S ek state function hai, do states ke beech Δ S sirf endpoints par depend karta hai, kabhi bhi path par nahi.
Definition Clausius inequality (master statement)
Kisi bhi cyclic process ke liye,
∮ T surr δ Q ≤ 0
equality sirf reversible cycle ke liye hai. Isse kisi bhi process A → B ke liye central result milta hai:
Δ S system ≥ ∫ A B T surr δ Q
aur universe ke liye (system + surroundings, isolated maana gaya):
Δ S univ ≥ 0
> 0 irreversible ke liye, = 0 reversible ke liye.
Δ S system aur Δ S univ — ye do alag cheezein kyun hain?
Δ S system akela negative ho sakta hai (jaise gas ko cool karna, paani freeze karna). Law yeh nahi hai ki "system entropy hamesha badhti hai." Law yeh hai ki "universe entropy hamesha badhti hai." Ise bhool jaana #1 trap hai.
Intuition "Irreversible ⇒ strictly greater" kyun hai
Irreversibility = uncontrolled gradients (temperature difference, pressure difference, friction, free expansion). Har aisa gradient work extract karne ka mauka "waste" karta hai aur balki entropy manufacture karta hai. Entropy production σ ≥ 0 define karo:
d S system = T surr δ Q + ≥ 0 δ σ
δ σ = 0 sirf tab jab har driving force infinitesimal ho (reversible). Real gradients finite hote hain, isliye σ > 0 .
Worked example (1) Ideal gas ki vacuum mein free expansion
Gas at T apna volume double karta hai V → 2 V vacuum mein. Adiabatic (Q = 0 ), koi work nahi (p ext = 0 ), to Δ U = 0 ⇒ T unchanged.
Naive trap: "Q = 0 , to Δ S = Q / T = 0 ." GALAT — us formula ko reversible path chahiye.
Sahi tarika: Unh'hin do endpoints ko ek reversible isothermal expansion se connect karo:
Δ S sys = ∫ T δ Q rev = T 1 ∫ V 2 V p d V = n R ln V 2 V = n R ln 2 > 0.
Ye step kyun? S ek state function hai — ek hi do states ke beech koi bhi reversible path lo.
Surroundings unchanged (Q = 0 ): Δ S surr = 0 .
Δ S univ = n R ln 2 > 0. ✔ Irreversible, strictly positive.
Worked example (2) Hot se cold body mein heat flow
Heat Q ek hot reservoir T H se cold reservoir T C mein flow karti hai (T H > T C ).
Δ S univ = hot loses − T H Q + cold gains + T C Q = Q ( T C 1 − T H 1 ) > 0.
Ye step kyun? Har reservoir apne T par reversibly heat exchange karta hai; sign = heat ki direction. Kyunki T C < T H , bracket positive hai.
Pehle forecast, phir verify: agar T H = T C , bracket = 0 → reversible limit. Match karta hai: equal temperatures = koi driving gradient nahi. ✔
Worked example (3) Warm room mein ice ka melt hona
m = 0.018 kg ice, T m = 273 K par melt hoti hai, room T room = 298 K par hai. Latent heat L = 334 kJ/kg, to Q = m L = 6012 J ice mein flow karti hai.
System (ice→water) Q ko 273 K par absorb karta hai (phase change constant T par):
Δ S sys = 273 Q = + 22.0 J/K .
Room Q ko 298 K par lose karta hai:
Δ S surr = − 298 Q = − 20.2 J/K .
Δ S univ = 22.0 − 20.2 = + 1.8 J/K > 0. ✔
Ye step kyun? Heat room ke T par leave karti hai lekin ice ke (lower) T par enter karti hai; same Q chhote T se zyada entropy gain deta hai jo loss se bada hota hai.
Common mistake "Har cheez ki entropy hamesha badhti hai."
Ye sahi kyun lagta hai: second law generally "entropy increases" ki tarah quote hoti hai.
Fix: sirf Δ S univ ≥ 0 . Ek system entropy lose kar sakta hai (paani freeze karna, gas compress karna) jab tak surroundings kam se kam utna gain karein.
Q = 0 to Δ S = 0 ."
Ye sahi kyun lagta hai: d S = δ Q / T , aur Q = 0 .
Fix: woh formula reversible path par δ Q rev use karta hai. Free expansion mein Q = 0 phir bhi Δ S = n R ln 2 > 0 . Δ S hamesha ek imaginary reversible path along evaluate karo same endpoints ke beech.
Common mistake "Surroundings ke liye
∫ δ Q / T mein system ka temperature use karo."
Ye sahi kyun lagta hai: ek process, ek temperature, natural lagta hai.
Fix: boundary ko irreversibly cross karne wali heat finite Δ T se bridge hoti hai. Surroundings ko T surr par aur system ko apne T par score karo. Ye mismatch exactly woh hai jo σ > 0 banata hai.
Common mistake "Irreversible ka matlab sirf slow vs fast hai."
Ye sahi kyun lagta hai: irreversible processes aksar fast hote hain.
Fix: irreversibility = finite gradients/dissipation (friction, mixing, finite Δ T /Δ p ). Friction ke saath ek quasi-static process phir bhi irreversible hai.
Recall Quick self-test (chhupao aur jawab do)
Precise second-law inequality batao. → Δ S univ ≥ 0 , > 0 agar irreversible.
Free expansion ke liye Δ S = Q / T kyun use nahi kar sakte? → Q reversible nahi tha; ek reversible isothermal path use karo.
Δ S univ = 0 kab hota hai? → reversible process (saare gradients infinitesimal).
Kya Δ S system < 0 ho sakta hai? → haan, agar surroundings zyada gain karein.
Recall Feynman: ek 12-saal ke bachche ko samjhao
Socho ek saathe box hai jisme red aur blue marbles hain, sab sort kiye hue. Use hilao — woh mix ho jaate hain aur tum unhe sirf aur hilane se kabhi perfectly sort nahi kar paoge. "Mixing" aasaan hai, "un-mixing" chance se practically kabhi nahi hoti. Entropy ek score hai ki cheezein kitni mixed-up / spread-out hain. Jab bhi kuch real hota hai — heat flow karna, gas spread karna, ice melt hona — poori duniya ka total mess score thoda badhta hai. Woh kabhi apne aap nahi ghatta. Yeh "kabhi nahi ghatta" rule hi wajah hai ki time ka ek direction hai: tum milk spill kar sakte ho lekin woh cup mein wapas nahi jaayega.
"U Never Drops" — U niverse ki entropy Never D ecreases. Aur trap ke liye: "Reversible = Reference (zero), Real = Rises."
Clausius inequality for any cycle ∮ δ Q / T surr ≤ 0 , equality iff reversible.
Definition of entropy change d S = δ Q rev / T ; S is a state function.
Second law in entropy form Δ S univ ≥ 0 ; strictly > 0 for irreversible processes.
Can system entropy decrease? Yes, if surroundings increase by at least as much so Δ S univ ≥ 0 .
Δ S for ideal-gas free expansion V → 2 V n R ln 2 > 0 (computed via reversible isothermal path).
Why Δ S = Q / T in free expansion Q is not reversible; entropy needs a reversible path between same endpoints.
Δ S univ for heat Q from T H to T C Q ( 1/ T C − 1/ T H ) > 0 .
Condition for Δ S univ = 0 Reversible process (all driving gradients infinitesimal).
Entropy production σ meaning d S = δ Q / T surr + δ σ , with δ σ ≥ 0 ; the irreversible part.
What is irreversibility physically Finite gradients/dissipation: friction, mixing, finite Δ T or Δ p , free expansion.
Entropy is a state function
Clausius definition dS = dQrev/T
Clausius inequality: cyclic dQ/T <= 0
Build cycle: irreversible A-B + reversible B-A
Split integral over two legs
Reversible leg = -delta S system
delta S system >= integral dQ/Tsurr
Irreversible: delta S univ > 0
Reversible: delta S univ = 0
System entropy alone can be negative