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Physics · Ch 2 — Kinematics

Differential Calculus

2.8

Differential Calculus

Any physical quantity that changes with another (usually time) is represented mathematically by a function. Temperature through the day is written T(t)T(t) — 'temperature as a function of time' — meaning that once a particular time tt is given, the function T(t)T(t) returns the temperature at that instant. In exactly the same way, the position of a particle moving along the xx-direction is written x(t)x(t), 'x as a function of time'.

More generally, if y=f(x)y=f(x), then yy is called the dependent variable and xx the independent variable: as xx changes, yy changes with it. Calculus is the branch of mathematics built to analyse exactly how a quantity changes as its independent variable changes, and the derivative dy/dxdy/dx is its central tool — it measures the instantaneous rate of change of yy with respect to xx. Formally,

dydx=lim⁡Δx→0y(x+Δx)−y(x)Δx=lim⁡Δx→0ΔyΔx\frac{dy}{dx} = \lim_{\Delta x\to 0}\frac{y(x+\Delta x)-y(x)}{\Delta x} = \lim_{\Delta x\to 0}\frac{\Delta y}{\Delta x}

Graphically, Δy/Δx\Delta y/\Delta x is the slope of the chord joining two nearby points on the curve y(x)y(x); as Δx\Delta x is shrunk towards (but never quite reaches) zero, that chord settles down to the tangent line at the point xx, and dy/dxdy/dx is the slope of that tangent. (It is important that Δx→0\Delta x\to 0 does not mean Δx=0\Delta x=0 — the ratio Δy/Δx\Delta y/\Delta x is undefined at Δx=0\Delta x=0, but it approaches a perfectly well-defined limiting value as Δx\Delta x gets arbitrarily small.)

A short table of derivatives used constantly in this chapter and beyond:

FunctionDerivative
y=xy=xdy/dx=1dy/dx = 1
y=x2y=x^2dy/dx=2xdy/dx = 2x
y=x3y=x^3dy/dx=3x2dy/dx = 3x^2
y=xny=x^ndy/dx=nxn−1dy/dx = nx^{n-1}
y=sin⁡xy=\sin xdy/dx=cos⁡xdy/dx = \cos x
y=cos⁡xy=\cos xdy/dx=−sin⁡xdy/dx = -\sin x
Figure 2.28Derivative of a function

What this figure shows. A smooth curve y(x)y(x) with a point PP on it; a small increment Δx\Delta x produces a rise Δy\Delta y, and as Δx\Delta x shrinks to zero the chord through PP becomes the tangent line at PP, whose slope is dy/dxdy/dx …