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Mathematics · Ch 5 — Continuity and Differentiability

Second Order Derivatives

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Second Order Derivatives

Definition. If y=f(x)y=f(x) is differentiable, its derivative dy/dx=f′(x)dy/dx=f'(x) is itself a function

of xx; if that function is in turn differentiable, its derivative is called the second order derivative (or second derivative) of yy with respect to xx, written

d2ydx2=ddx ⁣(dydx),or equivalentlyy′′=f′′(x).\frac{d^2y}{dx^2} = \frac{d}{dx}\!\left(\frac{dy}{dx}\right), \qquad\text{or equivalently}\qquad y''=f''(x).

Physically, if y=s(t)y=s(t) is the position of a particle at time tt, then dy/dtdy/dt is its velocity

and d2y/dt2d^2y/dt^2 is its acceleration -- the rate of change of the rate of change; more

generally, d2y/dx2d^2y/dx^2 measures how the slope of the curve y=f(x)y=f(x) itself is changing.

For an explicit function. If y=f(x)y=f(x) is given explicitly, finding y′′y'' is simply a matter

of differentiating twice in succession: find y′=dy/dxy'=dy/dx first, then differentiate that result

again with respect to xx.

For an implicitly-defined function. If yy is defined implicitly by an equation (Section 5),

the first derivative dy/dxdy/dx typically comes out as an expression in both xx and yy; to find

d2y/dx2d^2y/dx^2, differentiate this first-derivative expression again with respect to xx, using the

product/quotient rule as needed and substituting dy/dxdy/dx (already found) wherever a yy-term is

differentiated. For x2+y2=25x^2+y^2=25 (Example 5), dy/dx=−x/ydy/dx=-x/y, so

d2ydx2=ddx ⁣(−xy)=−y⋅1−x⋅(dy/dx)y2=−y−x(−xy)y2=−y+x2yy2=−x2+y2y3=−25y3,\frac{d^2y}{dx^2} = \frac{d}{dx}\!\left(-\frac{x}{y}\right) = -\frac{y\cdot1 - x\cdot(dy/dx)}{y^2} = -\frac{y - x\left(-\dfrac{x}{y}\right)}{y^2} = -\frac{y+\dfrac{x^2}{y}}{y^2} = -\frac{x^2+y^2}{y^3} = -\frac{25}{y^3},

using x2+y2=25x^2+y^2=25 in the last step to simplify the numerator back to a constant.

For a parametric function -- the one genuine trap. If x=f(t), y=g(t)x=f(t),\ y=g(t), the first derivative

is dy/dx=(dy/dt)/(dx/dt)dy/dx=(dy/dt)/(dx/dt) (Section 9), itself a function of tt. The second derivative is

not simply d2y/dt2d2x/dt2\dfrac{d^2y/dt^2}{d^2x/dt^2} -- that shortcut is a common and serious error.

Instead, treat dy/dxdy/dx as a new function of tt and apply the parametric-derivative idea a second

time:

d2ydx2=ddx ⁣(dydx)=ddt ⁣(dydx)dxdt.\frac{d^2y}{dx^2} = \frac{d}{dx}\!\left(\frac{dy}{dx}\right) = \frac{\dfrac{d}{dt}\!\left(\dfrac{dy}{dx}\right)}{\dfrac{dx}{dt}}. …