The differential turns the idea of an “infinitesimal variation along the tangent” into a self-standing object: it is the tool with which one approximates ff near a point and with which the notation dfdx\frac{df}{dx} acquires a precise meaning.

Definition — The differential

The differential of ff at the point xx with increment dxdx is: df=f(x)dx.df = f'(x)\cdot dx. Here dxdx is an infinitesimal increment of the independent variable (it is the same Δx\Delta x in the limit Δx0\Delta x\to 0, but written with a “d” to indicate that we have already passed to the limit). The differential dfdf is the approximate variation of ff along the tangent.

Remark — Why the notation dfdx\frac{df}{dx} makes sense

If one divides the differential df=f(x)dxdf = f'(x)\cdot dx by dxdx, one obtains dfdx=f(x)\frac{df}{dx} = f'(x). This is why the derivative can be “read” as a ratio between the differential of the function and the differential of the variable: it is not an abuse of notation but a genuine property of differentials.

Remark — The differential as an approximation

Geometrically, dfdf is the vertical displacement along the tangent line when one moves by dxdx horizontally. The true function moves by Δf=f(x+dx)f(x)\Delta f = f(x+dx)-f(x), slightly different from dfdf (the difference is an “error” of order dx2dx^2). But for small dxdx, dfΔfdf\approx\Delta f is an excellent approximation.

Topics: Derivatives
Concepts: Derivative · Differential · Leibniz notation
Skills: Estimating