2.4.6 · Physics › Thermodynamics & Statistical Mechanics (Advanced)
Jab do phases (maano liquid aur vapour) coexist karti hain, toh woh pressure–temperature plane mein ek single curve P ( T ) par baithe hote hain. Clausius-Clapeyron equation tumhe us coexistence curve ki slope batati hai.
YEH KYU HONA CHAHIYE: phases ke beech equilibrium koi ek point par ittefaq nahi hai — T ko thoda change karo aur phases tab bhi coexist kar sakti hain, lekin sirf tab jab P bilkul sahi amount se change ho. Woh "bilkul sahi amount" hi d T d P hai, aur thermodynamics ise latent heat aur volume change ke terms mein poori tarah se pin down kar deti hai.
Definition Coexistence condition
Ek hi substance ki do phases 1 aur 2 equilibrium mein hoti hain jab woh ek hi temperature, pressure, AUR chemical potential (specific Gibbs free energy) share karti hain:
T 1 = T 2 , P 1 = P 2 , μ 1 ( T , P ) = μ 2 ( T , P )
Chemical potential KYU? μ Gibbs free energy per particle (ya per mole) hai. Agar μ 1 < μ 2 ho, toh particles total Gibbs energy G ko kam karne ke liye phase 2 se phase 1 mein flow karte hain — toh phase 2 khatam ho jaata hai. Equilibrium (fixed T , P par koi net flow nahi) ke liye μ 1 = μ 2 zaroori hai. Yeh akela equation μ 1 ( T , P ) = μ 2 ( T , P ) , ( T , P ) plane mein ek curve define karta hai, koi area nahi: yahi coexistence line hai.
Step — d μ kyun use karein? Kyunki jab hum curve par chalte hain toh dono phases equal rehni chahiye; equal values + agli step par bhi equal ⇒ equal infinitesimal changes.
Ab humein d μ chahiye. Per mole Gibbs free energy g = μ se, fundamental relation (per mole) hai:
d g = − s d T + v d P
jahan s = molar entropy, v = molar volume.
d g = − s d T + v d P kyun?
Start karo G = U − T S + P V se. Tab d G = d U − T d S − S d T + P d V + V d P . Substitute karo first law d U = T d S − P d V . T d S aur − P d V khoobsurati se cancel ho jaate hain, aur bachta hai d G = − S d T + V d P . Per mole: d g = − s d T + v d P . Yeh cancellation hi wajah hai ki G , T aur P ka natural function hai.
Apply karo d μ 1 = d μ 2 :
− s 1 d T + v 1 d P = − s 2 d T + v 2 d P
Terms group karo:
( v 1 − v 2 ) d P = ( s 1 − s 2 ) d T
d T d P = v 2 − v 1 s 2 − s 1 = Δ v Δ s
Step — Yeh pehle se hi answer kyun hai: coexistence curve ki slope, phases ke beech entropy jump aur volume jump ka ratio hoti hai.
Δ s = L / T KYU? Latent heat transition ke dauran isothermally aur reversibly absorb hoti hai, isliye Δ S = ∫ d q r e v / T = L / T kyunki T constant hai. Yeh exact Clausius-Clapeyron equation hai — abhi tak koi approximation nahi .
Step — ln P vs 1/ T linear kyun hai: rewrite karo, ln P = − R L ⋅ T 1 + C . ln P ko 1/ T ke against plot karo toh slope − L / R wali straight line milti hai — latent heat measure karne ka standard experimental tarika.
Worked example Example 1 — Altitude par paani ka boiling point
Sea level par paani 373 K par, P 1 = 101.3 kPa par ubalata hai. L v a p = 40.7 kJ/mol. Boiling point dhundo jahan P 2 = 70 kPa ho.
Use karo ln P 1 P 2 = − R L ( T 2 1 − T 1 1 ) .
Yeh form kyun? Vapour phase hai, bada Δ v hai, isliye integrated vapour formula apply hota hai.
ln 101.3 70 = − 8.314 40700 ( T 2 1 − 373 1 )
LHS = ln ( 0.691 ) = − 0.369 . Toh − 0.369 = − 4895 ( T 2 1 − 2.681 × 1 0 − 3 ) .
T 2 1 − 2.681 × 1 0 − 3 = 7.54 × 1 0 − 5 ⇒ T 2 1 = 2.757 × 1 0 − 3 ⇒ T 2 ≈ 363 K.
Sanity check: kam pressure → kam boiling point. ✓ (pahaad par paani ~90 °C par ubalata hai).
Worked example Example 2 — Ice ka melting curve slope (woh anomaly)
Ice→water ke liye 0° C par (T = 273 K): L f u s = 6.01 kJ/mol, molar volumes v w a t er = 18.0 × 1 0 − 6 , v i ce = 19.66 × 1 0 − 6 m 3 /mol .
Δ v = v w a t er − v i ce = − 1.66 × 1 0 − 6 m 3 /mol ( negative! )
Negative kyun? Ice, water se kam dense hoti hai — freeze hone par yeh expand karti hai. Yahi famous water anomaly hai.
d T d P = T Δ v L = 273 × ( − 1.66 × 1 0 − 6 ) 6010 ≈ − 1.33 × 1 0 7 Pa/K
Interpretation: melting curve ka slope negative hai — pressure badhane se ice ka melting point kam hota hai. Isliye pressure skating mein thodi help kar sakta hai (chota sa effect) aur deep glaciers base par melt karte hain.
Worked example Example 3 —
ln P vs 1/ T plot se latent heat estimate karna
Maano ln P vs 1/ T ka measured slope − 5000 K hai.
Kyunki slope = − L / R hai: L = 5000 × 8.314 = 41.6 kJ/mol.
Yeh 80/20 move kyun hai: CC ki experimental power mostly isi single linear fit mein hai — do pressures measure karo, do temperatures measure karo, L mil jaayega.
Δ v hamesha positive hota hai."
Yeh sahi kyun lagta hai: zyada temperature wale phase ka volume usually zyada hota hai (gas > liquid), isliye hum d P / d T > 0 expect karte hain.
Fix: paani ke liye, v i ce > v w a t er hai, isliye Δ v < 0 aur slope ka sign palat jaata hai. Δ v ko hamesha v f ina l − v ini t ia l rakho, usi direction mein jis direction mein tumhara L hai (heat into same final phase).
Common mistake Melting ke liye ideal-gas integrated form use karna.
Yeh sahi kyun lagta hai: formula ln P 2 / P 1 = − R L ( … ) wahi hai jo sabko yaad hota hai.
Fix: woh form assume karta hai Δ v ≈ v g a s = R T / P — yeh sirf tab valid hai jab ek phase vapour ho . Solid–liquid ke liye, koi bhi phase gas nahi hai, isliye exact d T d P = T Δ v L use karo actual volumes ke saath.
Common mistake Yeh bhool jaana ki
L , T par depend karta hai.
Yeh sahi kyun lagta hai: agar L constant ho toh integration easy hai.
Fix: integrated log form assume karta hai ki L constant hai. Large T ranges par L vary karta hai; precision ke liye L ( T ) ko properly integrate karo. Exam-level problems ke liye constant L theek hai.
Recall Feynman style: ek 12 saal ke bacche ko samjhao
Socho ice aur paani ke beech ek tug-of-war chal raha hai. Woh 0° C par exactly tie karte hain. Agar temperature ko thoda change karo, toh tie toot jaati hai — jab tak tum unhe sahi amount mein squeeze nahi karte (pressure change nahi karte) taaki tie bani rahe. Clausius-Clapeyron equation woh rulebook hai jo kehti hai "tie banaye rakhne ke liye jab temperature 1 degree badhta hai, pressure ko itna change karo." Woh "itna" depend karta hai ki change kitni heat soak karta hai (latent heat) aur cheez kitni phailti ya sikarti hai (volume change). Paani weird hai: ice, paani se zyada jagah leti hai, isliye ise squeeze karna actually ise melt karne mein help karta hai.
Mnemonic Slope yaad rakho
"Love Tea, Very Slowly" → d T d P = T Δ v L : L ove (L) over T ea (T) times V olume (Δv). Aur log form ke liye: "Lin P vs one-over-T, slope is minus L-over-R."
Do phases coexist karne ke liye kaunsi teen quantities equal honi chahiye? Temperature T , pressure P , aur chemical potential μ (molar Gibbs free energy).
Exact Clausius-Clapeyron equation batao. d T d P = T Δ v L , jahan L molar latent heat hai aur Δ v molar volume change hai.
d g = − s d T + v d P kis cheez se derive hota hai?g = u − T s + P v se, d g = d u − T d s − s d T + P d v + v d P ; substitute karo d u = T d s − P d v ⇒ d g = − s d T + v d P .
Phase transition par Δ s = L / T kyun hota hai? Transition isothermal aur reversible hoti hai, isliye Δ s = ∫ d q r e v / T = L / T (T constant hai).
Vapour form d T d ln P = R T 2 L dene wale do approximations kya hain? (1) Δ v ≈ v g a s (liquid volume negligible hai); (2) vapour ideal hai, v g a s = R T / P .
Vaporisation ke liye ln P vs 1/ T plot ki slope kya hai? − L / R , latent heat measure karne ke liye use hota hai.
Ice ka d P / d T melting slope negative kyun hota hai? Kyunki v i ce > v w a t er hai isliye Δ v < 0 ; L > 0 ke saath, d P / d T < 0 — pressure ice ka melting point kam karta hai.
Zyada altitude par (kam pressure mein) paani ka boiling point badhta hai ya ghatta hai? Kyun? Ghatta hai; ln ( P 2 / P 1 ) = − R L ( 1/ T 2 − 1/ T 1 ) se, kam P ⇒ kam T b o i l .
delta s = L/T isothermal reversible
Chemical potential mu1 = mu2
dP/dT = delta s / delta v