3.3.22 · D1 · Physics › Rocket Propulsion › Staged combustion cycle — full flow, fuel-rich, oxidizer-ric
Ek rocket engine ek aisi machine hai jo propellant ko bahut zyada high-pressure wali aag mein dhakelta hai , aur us pressure ke khilaaf dhakelnay ka sirf ek hi tarika hai — ek pump jo hot-gas turbine se ghoomti hai . Parent page ke har symbol (m ˙ , Δ p , ρ , c p , T , γ , π t , η ) ka kaam ek sawaal ka jawaab dena hai: kya turbine itni power bana sakti hai ki pump chal sake?
Is page pe assume kiya gaya hai ki tumhe kuch bhi nahi pata . Hum har letter ko earn karenge — parent note ko use karne ki permission tabhi milegi. Upar se neeche padho — har idea agley ka foundation hai.
Definition Mass flow rate
m ˙ (padho "m-dot") woh mass of propellant hai jo har second ek point se guzarta hai , kilograms per second (kg/s ) mein measure hota hai. Upar wali dot ka matlab hamesha "per second" hota hai — yeh ek rate hai.
Socho tum ek moti pipe ke paas stopwatch lekar khade ho. Ek second mein liquid oxygen ka ek tukda tumhare paas se guzar jaata hai. Us tukde ko tolo — woh number hi m ˙ hai. Agar har second 500 kg guzre, toh m ˙ = 500 kg/s .
Topic ko iski zaroorat kyun hai: thrust literally hai "tum kitni tezi se mass ko peeche phenkte ho," isliye har power aur thrust equation m ˙ se shuru hoti hai. Dekho Rocket thrust equation .
ρ (Greek letter "rho", dekhne mein lowercase p ki tarah hai ek tail ke saath) yaani ek cubic metre mein kitna mass packed hai , kg/m 3 mein. Liquid oxygen dense hai: ρ LOX ≈ 1140 kg/m 3 — ek cubic metre ka wazan 1140 kg hoga.
Do identical 1-litre bottles: ek paani se bhari, ek liquid hydrogen se bhari. Paani wali bottle kaafi bhaari hai. Density matlab hai tumhari bottle ka wazan — bas itna hi.
1/ ρ mein palat dete hain
Agar ρ hai "mass per cubic metre," toh 1/ ρ hai "cubic metres per kilogram" — yaani ek kilogram kitna volume leta hai . Ek pump volume move karta hai, isliye jab hum mass flow m ˙ track karte hain toh ise volume flow mein convert karte hain m ˙ / ρ se. Yeh yaad rakho: yahi pump-power formula ke peeche ka trick hai.
Pressure p yaani force ek area pe faila hua , pascals mein: 1 Pa = 1 N/m 2 . Engineers bar bhi use karte hain: 1 bar = 1 0 5 Pa , roughly sea level pe atmospheric pressure ke barabar.
Intuition Picture — pressure yaani volume per stored energy
Neeche wala piston dekho. Pressure p ke khilaaf area A ki ek wall ko distance d tak dhakelo: force hai p ⋅ A , aur work = force × distance = p A d . Lekin A d sirf woh volume hai jo sweep hua. Toh
work = p × volume ⟹ p = volume energy .
Isliye parent note kehta hai "Pa = J/m 3 ." Ek pascal yaani joules per cubic metre. Yeh ek equivalence poore power balance ki neenv hai.
Δ p
Triangle Δ ("delta") ka matlab hai "mein change." Toh Δ p = p out − p in yaani pump ne pressure kitna boost kiya . Agar pump propellant ko 5 bar se 305 bar tak le jaaye, toh Δ p = 300 bar = 3 × 1 0 7 Pa .
Topic ko iski zaroorat kyun hai: chamber high pressure p c par hoti hai; pump ka poora kaam woh Δ p supply karna hai jo propellant ko us mein force karne ke liye chahiye. Zyada p c → bada Δ p → mushkil pump ka kaam. Yeh seedha Specific impulse and chamber pressure se jud ta hai.
Intuition Formula ko pictures se banana
Ek cubic metre ko andar dhakelnay ki energy = Δ p (§3 se: pascals hi hain joules per cubic metre).
Cubic metres flowing per second = m ˙ / ρ (§2 se: mass flow ko volume flow mein badla).
Multiply karo: energy-per-volume × volume-per-second = energy per second = power .
P pump = m ˙ ⋅ ρ 1 ⋅ Δ p = ρ m ˙ Δ p
Power P yaani har second deliver ki gayi energy , watts mein (1 W = 1 J/s ). Ek megawatt (MW ) yaani ek million watts. Ek bada rocket pump tens of MW maangta hai — ek choti power station ki power, ek microwave ke size ke box mein.
Topic ko iski zaroorat kyun hai: yeh cycle ka "demand" side hai — pumps power maangti hain, aur turbine ko woh supply karni padti hai.
η (Greek "eta", dekhne mein curly n jaisa) ek 0 aur 1 ke beech ka fraction hai jo bataata hai ki ideal work ka kitna hissa tumhe actually milta hai . η p = 0.7 wala pump 30% heat aur noise mein waste karta hai; η t = 0.75 wali turbine gas ki ideal energy ka sirf 75% capture karti hai.
Socho ek leaky bucket-chain paani utha rahi hai. Tum 10 buckets effort daalte ho; sirf 7 upar pahunchte hain. Woh "7 out of 10" hi η hai. Kyunki ek pump energy kho ta hai, tumhe ideal se zyada feed karna padta hai — isliye η p denominator mein baithta hai:
P pump = ρ η p m ˙ Δ p .
Kyunki turbine gas ki poori energy pakad nahi paati , uska useful output chota hota hai — isliye η t turbine power par ek multiplier ke roop mein baithta hai. Yaad rakho: denominator demand ko bada karta hai, multiplier supply ko chota karta hai. Dono tumhein hurt karte hain — iska matlab hi hai "real machine."
T yaani gas kitni hot hai , in formulaon ke liye hamesha kelvin (K ) mein. Kelvin absolute zero se shuru hoti hai, isliye kabhi negative numbers nahi aate jo maths tod dein. Room temperature ≈ 300 K ; stoichiometric LOX/LH₂ flame ≈ 3300 K .
c p
c p yaani constant pressure par gas ke ek kilogram ko ek kelvin garam karne mein kitne joules lagte hain , J / ( kg ⋅ K ) mein. Hydrogen ek champion heat-sponge hai: pure H₂ ke liye c p ≈ 14000 J / ( kg K ) , H₂-rich gas ke liye bhi hazaron.
c p T har jagah kyun aata hai
"Joules per kg per kelvin" ko "kelvin" se multiply karo aur kelvins cancel ho jaate hain:
c p T = kg ⋅ K J × K = kg J .
Toh c p T yaani hot gas ke har kilogram mein stored heat energy — turbine ke liye tank mein fuel. Gas jitni zyada garm ho (T ) aur jitni zyada spongy ho (c p ), har kilogram turbine blades tak utni zyada energy carry karta hai.
Intuition "Rich burning" flame temperature kyun giraa deti hai — ek line mein
Chemical energy released Q fixed hai, lekin temperature rise hai Δ T = Q / ( m c p ) . Extra hydrogen daalo: m badhta hai aur c p badhta hai (H₂ spongy hai), toh wahi Q ek chota Δ T produce karta hai . Yahi poori wajah hai ki ek preburner off-stoichiometric chalti hai — dekho Combustion stoichiometry and flame temperature .
Definition Pressure ratio
π t (yahan sirf ek letter hai, 3.14159 nahi) yaani turbine inlet pressure divided by outlet pressure :
π t = p out p in .
Agar gas 450 bar par enter kare aur 300 bar par nikle, toh π t = 1.5 . Yeh hamesha > 1 hota hai kyunki gas ko energy dene ke liye pressure drop karna padta hai.
Intuition Picture — gas ek paddle-wheel ko dhakelta hai
Hot gas turbine se guzar ke expand hoti hai. Expanding gas blades par dhakelta hai — woh push shaft ko ghoomata hai. Jitna bada pressure drop (bada π t ), gas utni zyada expand hoti hai, utna zyada dhakelta hai. Parent ka bracket
[ 1 − π t − ( γ − 1 ) / γ ]
exactly woh fraction hai jo gas ki heat energy ka ek perfect expansion shaft work mein convert karta hai . Jab π t = 1 ho (koi drop nahi) toh bracket 0 hai — koi push nahi, koi power nahi. π t badhne ke saath bracket 1 ki taraf barhta hai.
γ (Greek "gamma") yaani do specific heats ka ratio , γ = c p / c v . Zyaadatar rocket gases ke liye γ ≈ 1.2 –1.4 . Yeh hamesha > 1 hota hai aur iska koi unit nahi hota.
Intuition Yeh exponent mein kyun rehta hai
γ decide karta hai ki jab gas expand hoti hai bina heat khoye (ek adiabatic expansion — koi heat leak nahi hoti) toh pressure aur temperature kaise trade off hote hain. Zyada springy gas (zyada γ ) expand hote waqt zyada tezi se thandi hoti hai, isliye energy alag tarike se deti hai. Combination ( γ − 1 ) / γ exactly woh exponent hai jo nature us trade ke liye use karta hai — tumhe yahan ise derive nahi karna, sirf yeh jaanna hai ki yeh gas se set ek fixed number hai , roughly 0.286 jab γ = 1.4 ho.
power balance turbine equals pump
Khud ko test karo — right side cover karo aur aawaaz mein jawaab do.
m ˙ mein dot ka hamesha kya matlab hota hai?"per second" — yeh ek rate batata hai, yahan kg per second.
Hum pressure ko J/m³ kyun likh sakte hain? Kyunki work = pressure × volume, isliye pressure = energy per volume (Pa = J/m 3 ).
1/ ρ physically kya hai?Woh volume jo ek kilogram occupy karta hai (m³/kg) — yeh mass flow ko volume flow mein convert karta hai.
Δ p ka kya matlab hai aur pump ko iska kyun khayal hai?Pressure boost p o u t − p in ; pump ko yeh supply karni padti hai taaki propellant ko high-pressure chamber mein force kiya ja sake.
η p denominator mein kyun baithta hai lekin η t multiplier ke roop mein?Ek real pump ko zyada input chahiye (÷ by <1 ise badhata hai); ek real turbine kam output deti hai (× by <1 ise ghataata hai).
Product c p T kya represent karta hai? Gas ke har kilogram mein stored heat energy (J/kg) — turbine ki fuel supply.
Rich burning flame temperature kyun giraata hai? Δ T = Q / ( m c p ) ; extra reactant m aur c p dono badhata hai, isliye wahi Q ek chota temperature rise deta hai.
π t kya hai aur yeh hamesha > 1 kyun hota hai?Inlet-over-outlet pressure; gas ko energy release karne ke liye pressure drop karna padta hai, isliye out < in.
Bracket 1 − π t − ( γ − 1 ) / γ kya hoga jab π t = 1 ho? Zero — koi pressure drop nahi matlab koi expansion nahi, koi shaft work nahi.
Power balance ek sawaal ka jawaab deta hai? Kya turbine exactly woh power produce karti hai jo pumps maangti hain?
Parent topic: Staged combustion cycle · Neighbours: Gas-generator cycle , Expander cycle , Turbopump design , Regenerative cooling