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Mathematics · Ch 10 — Differential Calculus – Differentiability and Methods of Differentiation

Higher order Derivatives

10.4.8

Higher order Derivatives

If s=s(t)s=s(t) is the position (displacement) of an object moving along a straight line, its first derivative already has a direct physical meaning: the velocity v(t)=s′(t)=dsdt=lim⁡Δt→0s(t+Δt)−s(t)Δtv(t) = s'(t) = \dfrac{ds}{dt} = \lim_{\Delta t\to0}\dfrac{s(t+\Delta t)-s(t)}{\Delta t} — this is exactly the instantaneous velocity defined in §10.2.2. The instantaneous rate of change of velocity with respect to time is called the acceleration a(t)a(t) of the object; being the derivative of v(t)v(t), it is therefore the second derivative of the position function:

a(t)=v′(t)=ddt[v(t)]=ddt ⁣(dsdt)=d2sdt2=s′′(t).a(t) = v'(t) = \frac{d}{dt}\big[v(t)\big] = \frac{d}{dt}\!\left(\frac{ds}{dt}\right) = \frac{d^2s}{dt^2} = s''(t).

More generally, for any differentiable function ff, the first derivative f′(x)f'(x) is itself a function of xx and so may itself have a derivative — if it exists, it is denoted f′′=(f′)′f''=(f')' and called the second derivative:

f′′(x)=lim⁡Δx→0f′(x+Δx)−f′(x)Δx=ddx ⁣[ddxf(x)]=d2fdx2=d2ydx2.f''(x) = \lim_{\Delta x\to0}\frac{f'(x+\Delta x)-f'(x)}{\Delta x} = \frac{d}{dx}\!\left[\frac{d}{dx}f(x)\right] = \frac{d^2f}{dx^2} = \frac{d^2y}{dx^2}.

Other equivalent notations: D2f(x)D^2f(x), D2yD^2y, y′′y''. Geometrically, while f′f' has the simple reading "slope of the tangent", the second derivative measures a rate of change of a rate of change; its geometric meaning is subtler (it connects, in later study, to the radius of curvature of the graph), but the physical reading — acceleration, when yy is position — is immediate.

Higher orders still. If f′′f'' itself is differentiable, its derivative is the third derivative, f′′′(x)=d3ydx3=y′′′f'''(x) = \dfrac{d^3y}{dx^3} = y'''. Physically, when y=s(t)y=s(t) is position, s′′′(t)=a′(t)s'''(t) = a'(t) is called the jerk: j=dadt=d3sdt3j = \dfrac{da}{dt} = \dfrac{d^3s}{dt^3} — the rate of change of acceleration, aptly named because a large jerk means a sudden change in acceleration, producing an abrupt jolt.

Worked illustration — explicit polynomial. For y=x3−6x2−5x+3y=x^3-6x^2-5x+3: y′=3x2−12x−5y'=3x^2-12x-5, then y′′=6x−12y''=6x-12, then y′′′=6y'''=6 (a constant — differentiating a cubic three times always eventually gives a constant, and a fourth derivative would be 00).

Worked illustration — a power with a negative exponent. For y=1/x=x−1y=1/x=x^{-1}: y′=−x−2y'=-x^{-2}, y′′=(−1)(−2)x3=2!x3y''=\dfrac{(-1)(-2)}{x^3}=\dfrac{2!}{x^3}, and y′′′=(−1)(−2)(−3)x4=−3!x4y'''=\dfrac{(-1)(-2)(-3)}{x^4}=-\dfrac{3!}{x^4} — each further derivative of x−1x^{-1} brings down one more factorial-growing constant with alternating sign.

Worked illustration — a product, needing product + chain rule twice. For f(x)=xcos⁡xf(x)=x\cos x: f′(x)=−xsin⁡x+cos⁡xf'(x) = -x\sin x+\cos x (product rule); differentiating again (product rule on −xsin⁡x-x\sin x, plus the derivative of cos⁡x\cos x), f′′(x)=−(xcos⁡x+sin⁡x)−sin⁡x=−xcos⁡x−2sin⁡xf''(x) = -(x\cos x+\sin x)-\sin x = -x\cos x-2\sin x.

Worked illustration — implicit second derivative. For x4+y4=16x^4+y^4=16: differentiating implicitly, 4x3+4y3y′=04x^3+4y^3y'=0, so y′=−x3/y3y'=-x^3/y^3. To find y′′y'', differentiate this expression for y′y' using the quotient rule, remembering yy is itself a function of xx: y′′=y3(−3x2)−(−x3)(3y2y′)y6=−3x2y3+3x3y2y′y6y'' = \dfrac{y^3(-3x^2)-(-x^3)(3y^2y')}{y^6} = \dfrac{-3x^2y^3+3x^3y^2y'}{y^6}; substituting y′=−x3/y3y'=-x^3/y^3 and simplifying yields y′′=−3x2y7(y4+x4)=−3x2(16)y7=−48x2y7y'' = -\dfrac{3x^2}{y^7}\big(y^4+x^4\big) = -\dfrac{3x^2(16)}{y^7} = -\dfrac{48x^2}{y^7} (using the original equation x4+y4=16x^4+y^4=16 to simplify). …