KTU S1

The Derivative as a Limit

By the end you should be able to: Define the derivative as a limit of difference quotients, interpret it as an instantaneous rate of change and as the slope of the tangent, and compute a derivative from first principles.

The derivative is not a new idea bolted onto limits. It is a limit — one specific limit that turns out to be useful everywhere.

From average to instantaneous

Between x=ax = a and x=a+hx = a + h, the average rate of change of ff is

f(a+h)−f(a)h\frac{f(a+h) - f(a)}{h}

This is the difference quotient: rise over run, the slope of the line joining the two points on the graph (the secant line).

Now shrink hh. The second point slides toward the first, the secant pivots, and in the limit you have the slope at a single point:

f′(a)=lim⁡h→0f(a+h)−f(a)hf'(a) = \lim_{h \to 0}\frac{f(a+h) - f(a)}{h}

That is the definition. When the limit exists, ff is differentiable at aa.

Why the limit is unavoidable

Setting h=0h = 0 directly gives f(a)−f(a)0=00\dfrac{f(a)-f(a)}{0} = \dfrac{0}{0} — indeterminate, exactly the form from the previous topic. A rate of change at a single instant is not something arithmetic can produce, because a single point has no run to divide by. The limit is what makes the question answerable.

Two readings of the same number

ReadingMeaning
GeometricSlope of the tangent to y=f(x)y=f(x) at x=ax=a
PhysicalInstantaneous rate of change of ff with respect to xx

If s(t)s(t) is position, s′(t)s'(t) is velocity and s′′(t)s''(t) is acceleration. The second derivative is the rate of change of the rate of change — which is why acceleration feels different from speed.

Differentiable implies continuous — not the reverse

If ff is differentiable at aa then ff is continuous at aa. The converse fails, and the standard counterexample is worth knowing:

f(x)=∣x∣at x=0f(x) = |x| \quad \text{at } x = 0

It is continuous there. But

lim⁡h→0−∣h∣−0h=−1,lim⁡h→0+∣h∣−0h=1\lim_{h\to 0^-}\frac{|h|-0}{h} = -1, \qquad \lim_{h\to 0^+}\frac{|h|-0}{h} = 1

The one-sided limits of the difference quotient disagree, so f′(0)f'(0) does not exist. The graph has a corner: no single tangent line.

Continuity is necessary for differentiability, not sufficient.

The alternative form

Sometimes written with x→ax \to a instead of h→0h \to 0:

f′(a)=lim⁡x→af(x)−f(a)x−af'(a) = \lim_{x\to a}\frac{f(x)-f(a)}{x-a}

Identical content, substituting x=a+hx = a + h. Use whichever makes the algebra shorter.

Notation

f′(x),dydx,ddxf(x),y˙f'(x), \qquad \frac{dy}{dx}, \qquad \frac{d}{dx}f(x), \qquad \dot{y}

All the same object. Leibniz's dy/dxdy/dx is suggestive of the difference quotient it came from, which is why it dominates in applied work.