f(x)=x2sin(1/x) (f(0)=0) is differentiable everywhere with f′(0)=0, yet the derivative f′(x)=2xsin(1/x)−cos(1/x) oscillates and is discontinuous at 0. Differentiable does not imply continuously differentiable — though derivatives still keep the intermediate value property (Darboux).
f′(0)=h→0limhsin(1/h)=0
f′(x)=2xsin(1/x)−cos(1/x)(x=0),f′(2πn1)=−1
Examples & Exercises
For f(x)=x2sin(1/x) (x=0), f(0)=0, prove completely by the squeeze theorem that f′(0)=0.
hf(h)−f(0)=hsinh1,hsinh1≤∣h∣→0
r=0.1, h=0.01: the difference quotient ≈−0.0051 is near 0, and the left panel shows the secant slope collapsing onto the horizontal (dashed) tangent.Show proof
By the definition of the derivative, f′(0)=limh→0hf(h)−f(0) (h=0). Since f(0)=0 and f(h)=h2sin(1/h) for h=0, the difference quotient simplifies to hh2sin(1/h)−0=hsin(1/h).
Since ∣sin(1/h)∣≤1, we have ∣hsin(1/h)∣≤∣h∣. As ∣h∣→0 (h→0), the squeeze theorem gives hsin(1/h)→0 — the limit of the difference quotient exists and f′(0)=0. The oscillating factor sin(1/h) is completely damped by the factor h.
In the scene, shrinking h down to 0.0001 shows the difference quotient converging to 0 numerically (alongside the bound ∣hsin(1/h)∣≤∣h∣).
Prove completely, via the product and chain rules, that f′(x)=2xsin(1/x)−cos(1/x) for x=0.
f′(x)=dxd[x2sinx1]=2xsinx1−cosx1(x=0)
r=0.1: the right panel plots exactly this formula — the 2xsin(1/x) term decays to 0 while the −cos(1/x) term keeps oscillating with amplitude 1.Show proof
Fix x=0. Since f(x)=x2⋅sin(1/x) is a product of differentiable functions, apply the product rule: f′(x)=2x⋅sin(1/x)+x2⋅dxdsin(1/x).
By the chain rule, dxdsin(1/x)=cos(1/x)⋅dxd(1/x)=cos(1/x)⋅(−1/x2) (since 1/x is differentiable at x=0). Substituting, f′(x)=2xsin(1/x)+x2⋅cos(1/x)⋅(−1/x2)=2xsin(1/x)−cos(1/x) — proved.
Numerical check: f′(0.5)=2(0.5)sin2−cos2≈1.3254, matching the model. This formula is not defined at x=0 — f′(0) must be computed separately as the limit of the difference quotient, as in problem 1.
Prove completely, using the sequence xn=1/(2πn), that f′ is discontinuous at x=0.
r=0.01, h=0.001: zooming closer to 0, the right panel never stops oscillating, and the highlighted points xn=1/(2πn) keep landing on the dashed line y=−1.Show proof
Set xn=1/(2πn); then xn=0 and xn→0. Plugging into problem 2's formula, f′(xn)=2xnsin(1/xn)−cos(1/xn)=2xnsin(2πn)−cos(2πn). Since sin(2πn)=0 and cos(2πn)=1, we get f′(xn)=0−1=−1 — constant for every n.
Hence f′(xn)→−1, but f′(0)=0 by problem 1, so f′(xn)→f′(0) even though xn→0. By the sequential criterion, f′ is not continuous at 0 — limx→0f′(x) does not even exist (the never-ending oscillation in the right panel).
Remark: a discontinuous derivative still has the intermediate value property — by Darboux's theorem, f′ satisfies the IVP on intervals. Differentiability is strictly weaker than continuity of the derivative.