Yeh step kyun?dL ko left side par le jaana aur group karna dikhata hai ki woh natural quantity jiska differential sirf dp, dq, dt involve karta hai, exactly H=∑piq˙i−L hai. Iske differential mein koi dq˙ nahi — proof hai ki H genuinely (q,p,t) ka function hai.
H=∑ipiq˙i−L, phir H(q,p,t) ki tarah express karo.
H=∑piq˙i−L likhne ke baad, aage kya KARNA ZAROORI hai?
pi=∂L/∂q˙i invert karke saare q˙i eliminate karo, taaki H sirf (q,p,t) par depend kare.
Kaunsa mathematical operation L ko H mein badalta hai?
Velocities q˙i ke saath Legendre transform.
Hamilton's canonical equations batao.
q˙i=∂H/∂pi aur p˙i=−∂H/∂qi.
Hamilton's equations kitni aur kis order ki hain Euler–Lagrange se compare mein?
2n first-order ODEs vs n second-order ODEs.
H total energy T+V ke barabar hone ki condition kya hai?
Tq˙ mein homogeneous quadratic ho (koi explicit-time/linear velocity terms nahi) AUR V velocity-independent ho.
H conserved hone ki condition kya hai?
∂H/∂t=0, equivalently ∂L/∂t=0 (koi explicit time dependence nahi).
Natural systems ke liye ∑piq˙i=2T kyun hota hai?
q˙i mein homogeneous quadratic T par Euler's theorem ki wajah se.
Aisa ek system batao jahan H conserved ho lekin H=E ho.
Uniformly rotating wire par bead (time-dependent constraint).
L ke terms mein ∂H/∂t kya hai?
∂H/∂t=−∂L/∂t.
Recall Feynman: ek 12-saal ke bachche ko explain karo
Ek chalte hua toy car describe karne ki soch. Tum track kar sakte ho "woh kahan hai aur kitna fast ja raha hai" (yahi Lagrangian tarika hai: position + speed). Ya tum track kar sakte ho "woh kahan hai aur kitna push carry karta hai" (yahi momentum hai — Hamiltonian tarika). Dono exactly wahi car describe karte hain! Hamiltonian ek clever recipe hai, H=pq˙−L, jo tumhe "speed" description se "push" description mein switch karti hai. Bonus: push-description mein, total energy usually seedhi tumhare saamne hoti hai, aur motion ke rules bahut simple ho jaate hain — ek neat rule position ke change ke liye, ek push ke change ke liye.