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Continuity and Differentiability

8 articles32 formulas40 ways the board asks it
MATSecond-Order Derivatives

Second-Order Derivatives

The second-order derivative d2ydx2\dfrac{d^2y}{dx^2} is the derivative of dydx\dfrac{dy}{dx} and measures curvature/concavity. A signature ISC theme is proving a differential equation that yy satisfies, by computing y′y' and y′′y'' and eliminating the constants.

These proofs often start from y=easin⁡−1xy=e^{a\sin^{-1}x} or y=(sin⁡−1x)2y=(\sin^{-1}x)^2 and rely on squaring relations to remove surds.

Definition
d2ydx2=ddx ⁣(dydx)\dfrac{d^2y}{dx^2} = \dfrac{d}{dx}\!\left(\dfrac{dy}{dx}\right)
y′′=d2ydx2y''=\dfrac{d^2y}{dx^2}; the derivative of the first derivative w.r.t. the same variable xx.
Harmonic relation
y=Asin⁡x+Bcos⁡x  ⇒  d2ydx2+y=0y = A\sin x + B\cos x \;\Rightarrow\; \dfrac{d^2y}{dx^2} + y = 0
A,BA,B arbitrary constants; differentiate twice and add to eliminate them.
Result for y=(sin⁡−1x)2y=(\sin^{-1}x)^2
(1−x2) y′′−x y′−2=0(1-x^2)\,y'' - x\,y' - 2 = 0
Start from (1−x2)(y′)2=4y(1-x^2)(y')^2=4y, differentiate once more and cancel 2y′2y'.
Result for y=easin⁡−1xy=e^{a\sin^{-1}x}
(1−x2) y′′−x y′−a2y=0(1-x^2)\,y'' - x\,y' - a^2 y = 0
1−x2 y′=ay\sqrt{1-x^2}\,y'=a y; square to remove the surd, then differentiate and simplify.
  • Compute y′y' first, then differentiate again (using product/quotient/chain rules) to get y′′y''.
  • To prove a differential equation, find y′y', often square or rearrange to eliminate surds/inverse-trig, then differentiate again.
  • For y=emtan⁡−1xy=e^{m\tan^{-1}x}: (1+x2)y′=my(1+x^2)y'=my, differentiating gives (1+x2)y′′+(2x−m)y′=0(1+x^2)y''+(2x-m)y'=0.
  • After differentiating a squared relation like (1−x2)(y′)2=ky(1-x^2)(y')^2=ky, divide through by the common factor 2y′2y' (valid where y′≠0y'\ne0).
  • Keep arbitrary constants until they cancel; the final differential equation should be free of them.
  • Watch the sign of the xy′x y' term: it is −xy′-x y' for the sin⁡−1\sin^{-1}-based functions above and +(2x−m)y′+(2x-m)y' for the emtan⁡−1xe^{m\tan^{-1}x} case.
  • Verify the order matches: an nn-constant family yields an nn-th order differential equation.
Where the marks go
  • Forgetting the chain rule on the second differentiation, especially with 1−x2\sqrt{1-x^2} or inverse-trig terms.
  • Sign errors in the xy′x y' term when eliminating constants.
  • Failing to square the first-derivative relation to clear the surd before differentiating again.
  • Leaving the arbitrary constants (AA, BB, aa, mm) in the final result instead of eliminating them.
How the board asks it
  • Derive / proveeliminating constants from y′y' and y′′y''
    If y=easin⁡−1xy = e^{a\sin^{-1}x}, prove that (1−x2)d2ydx2−xdydx−a2y=0(1-x^2)\dfrac{d^2y}{dx^2} - x\dfrac{dy}{dx} - a^2 y = 0.
  • Numericalproduct and chain rule
    If y=x3log⁡xy = x^3 \log x, find d2ydx2\dfrac{d^2y}{dx^2} and evaluate it at x=1x = 1.
  • Numericalparametric differentiation
    If x=a(θ+sin⁡θ)x = a(\theta + \sin\theta) and y=a(1−cos⁡θ)y = a(1 - \cos\theta), find d2ydx2\dfrac{d^2y}{dx^2} at θ=π2\theta = \dfrac{\pi}{2}.
  • Derive / proveemtan⁡−1xe^{m\tan^{-1}x} relation (1+x2)y′=my(1+x^2)y'=my
    If y=emtan⁡−1xy = e^{m\tan^{-1}x}, prove that (1+x2)d2ydx2+(2x−m)dydx=0(1+x^2)\dfrac{d^2y}{dx^2} + (2x - m)\dfrac{dy}{dx} = 0.
  • Derive / provecos⁡(log⁡x)\cos(\log x) and sin⁡(log⁡x)\sin(\log x) family
    If y=Acos⁡(log⁡x)+Bsin⁡(log⁡x)y = A\cos(\log x) + B\sin(\log x), show that x2d2ydx2+xdydx+y=0x^2\dfrac{d^2y}{dx^2} + x\dfrac{dy}{dx} + y = 0.

Practise this topic

Written for Sublevo. Question text quoted anywhere in these notes is the Council’s and carries its year and paper; the board’s own diagrams are not reproduced.