80/20 core: A linear 2nd-order PDE in two variables is classified by the sign of the discriminantB2−4AC. Negative → elliptic, zero → parabolic, positive → hyperbolic. This single sign tells you the physics, the boundary conditions you need, and the solution method.
We want to know: along which curves can a solution have a "kink" (discontinuity in 2nd derivatives)? Those curves are called characteristics. Their existence is the deep meaning of the classification.
Step 1 — Look for characteristic curves y=y(x).
Why? Because a PDE behaves like an ODE along special directions where the second derivatives are not fully determined by the data. Finding those directions tells us the type.
Suppose a curve ϕ(x,y)=const is a characteristic. Substitute ξ=ϕ as a new coordinate. The principal part transforms; the coefficient of uξξ becomes
Q(ϕx,ϕy)=Aϕx2+Bϕxϕy+Cϕy2.Why this expression? Because under a change of variables the chain rule sends uxx→ϕx2uξξ+…, uxy→ϕxϕyuξξ+…, uyy→ϕy2uξξ+…. Collecting uξξ gives exactly Q.
Step 2 — A characteristic is where this coefficient vanishes:Q=0.
Along ϕ=const we have dϕ=ϕxdx+ϕydy=0, so the slope is
dxdy=−ϕyϕx.
Divide Q=0 by ϕy2 and let m=ϕx/ϕy:
Am2+Bm+C=0⇒m=2A−B±B2−4AC.
The names echo conic sections Ax2+Bxy+Cy2=const, classified by the sameB2−4AC.
Which physical equation for each? (Laplace, Heat, Wave)
Linear vs quasilinear? (linear: coeffs depend only on x,y; quasilinear: top-derivative coeffs may depend on u and lower derivatives)
Recall Feynman: explain to a 12-year-old
Imagine dropping a pebble in three different worlds.
In the wave world, ripples shoot out along straight lines at a fixed speed — you can see exactly where the ripple front is. That's hyperbolic (two clear lines).
In the heat world, a drop of warm dye slowly blurs out, no sharp edge, just smearing as time goes on. That's parabolic (one smearing direction).
In the calm-pond world, the water is already perfectly still and every part of the surface gently balances every other part — no fronts, no smearing, just smooth equilibrium. That's elliptic.
The little number B2−4AC is a magic detector that tells you which world your equation lives in: negative = calm pond, zero = blurring dye, positive = shooting ripples.
Dekho, second-order PDE ko classify karna bahut simple hai agar tum sirf ek number pe dhyaan do: discriminantΔ=B2−4AC. Yahan A,B,C sirf second-order termsuxx,uxy,uyy ke coefficients hain — first-order ux,uy wale terms ko bilkul ignore karo, woh classification mein aate hi nahi. Bas sign dekho: Δ<0 matlab elliptic (Laplace), Δ=0 matlab parabolic (Heat), Δ>0 matlab hyperbolic (Wave).
Ek important baat: linear aur quasilinear ek nahi hote. Linear PDE mein saare coefficients (highest derivatives ke bhi) sirf independent variables x,y pe depend karte hain, u ya uske derivatives pe nahi. Quasilinear mein highest-order derivatives ke coefficients u aur uske lower-order derivatives pe depend kar sakte hain (par highest derivatives phir bhi linearly aate hain). Isliye quasilinear case mein type khud solution pe bhi depend kar sakta hai.
Ye discriminant aata kahan se hai? Hum poochte hain ki solution kis curve ke along "kink" rakh sakta hai — usko characteristic bolte hain. Calculation karne par ek quadratic milta hai Am2+Bm+C=0, aur uske real roots ki ginti Δ ke sign se decide hoti hai. Do real roots = hyperbolic, ek root = parabolic, koi real root nahi = elliptic.
Physics-wise: Wave mein signal fixed speed se sharp line ke along jaata hai (hyperbolic), Heat mein dye dheere-dheere blur hota hai (parabolic), aur Laplace mein paani bilkul shaant, har point har boundary point ko feel karta hai (elliptic). Common galti: Heat equation mein C=1 maan lena — galat! ut first order hai, utt hai hi nahi, to C=0 aur Δ=0. Aur Tricomi jaise equations mein coefficients x,y pe depend karte hain, to har point pe Δ evaluate karo.