Shuru karo oblique-shock geometry se. Maano β shock-wave angle hai aur θ uske peeche flow ka deflection hai. Upstream velocity ko shock ke normal (un) aur tangential (ut) components mein decompose karo.
θ–β–M relation ki derivation (taaki tum dekh sako θmax kahan se aata hai):
Upstream normal Mach number: Mn1=M1sinβ.
Kyun? Shock sirf apne perpendicular component ko "dekhti" hai, aur woh component, sound speed a1 se divide karke, M1sinβ hota hai.
Ek normal shock ke across, density ratio hai
ρ1ρ2=(γ−1)Mn12+2(γ+1)Mn12.Kyun? Shock ke across mass + momentum + energy exactly yahi deta hai (Rankine–Hugoniot result).
ut conserved use karke pehle/baad ke velocity triangles ki geometry:
tanβtan(β−θ)=un1un2=ρ2ρ1.Kyun?tanβ=un1/ut aur tan(β−θ)=un2/ut; divide karo, ut cancel ho jaata hai, aur mass conservation deta hai un2/un1=ρ1/ρ2.
(2) ko (3) mein substitute karo aur simplify karo standard θ–β–M relation mein:
tanθ=2cotβM12(γ+cos2β)+2M12sin2β−1
Jab required deflection θ, maximum oblique-shock deflection θmax(M1) se zyada ho jaaye.
Bow shock ki centreline par shock-wave angle β kya hota hai?
β=90° (wahan yeh normal shock ki tarah behave karta hai).
Bow shock ki centreline ke theek peeche flow subsonic hai ya supersonic?
Subsonic (M2<1).
Stand-off distance kya hota hai?
Detached shock aur body ke nose ke beech ka gap Δ.
M1 badhne par stand-off distance kaise change hota hai?
Yeh chhota hota hai (shock body ko hug karta hai), high Mach par ek chhoti finite value par tend karta hai.
Mathematically shock detach kyun hota hai?
θ–β–M relation ka θ>θmax ke liye koi real β solution nahi hota.
θ–β–M relation likho.
tanθ=2cotβM12(γ+cos2β)+2M12sin2β−1.
Mn1 ko M1 aur β ke terms mein kya hota hai?
Mn1=M1sinβ.
M1=2, γ=1.4 par θmax approximately kya hota hai?
Lagbhag 22.97°.
Oblique shock ke across tangential velocity kyun conserved rehti hai?
Shock sirf apne normal ke along act karti hai, isliye tangential component unchanged rehta hai.
Recall Feynman: 12-saal ke bachche ko samjhao
Socho tum bahut tez daud rahe ho aur apne aage ki air ko push kar rahe ho. Agar tumhara shape pointy arrow jaisa hai aur tum super fast ja rahe ho, to air seedha point ke saath fold ho sakti hai — yeh attached shock hai. Lekin agar tumhara front mota aur gol hai, to pile ho rahi air itni sharply bend nahi kar sakti ki tumhari shape follow kar sake. To woh haar maanti hai aur squished air ki ek curved wall bana deti hai jo tumhare theek aage float karti hai, jaise ek invisible bubble shield. Us shield ke bilkul beech mein air l거의 ruk jaati hai aur "sound speed" se neeche aa jaati hai, jisse woh calmly tumhare mote nose ke around slide ho sakti hai. Tez jao aur shield tumhare chehre se aur tight ho jaayegi.