TheoremBase

Proof

Throughout, differentiability at an interior point x0x_0 of II is the condition of Derivative at an Interior Point; its admissible increments are the real numbers hh with x0+h∈Ix_0+h\in I. Continuity is the condition of Continuity at a Point. We repeatedly use the triangle inequality for real numbers.

Claim 1. Write L=f′(x0)L=f'(x_0). Applying the definition of the derivative with ε=1\varepsilon=1, there is δ0>0\delta_0>0 such that for every admissible hh with 0<∣h∣<δ00<|h|<\delta_0,

∣f(x0+h)−f(x0)h−L∣<1,\Bigl|\frac{f(x_0+h)-f(x_0)}{h}-L\Bigr|<1,

hence ∣f(x0+h)−f(x0)∣≤(∣L∣+1)∣h∣|f(x_0+h)-f(x_0)|\le(|L|+1)|h|. Let ε>0\varepsilon>0 and put δ=min⁡(δ0, ε/(∣L∣+1))\delta=\min\bigl(\delta_0,\ \varepsilon/(|L|+1)\bigr). For x∈Ix\in I with ∣x−x0∣<δ|x-x_0|<\delta: if x=x0x=x_0 then ∣f(x)−f(x0)∣=0<ε|f(x)-f(x_0)|=0<\varepsilon; otherwise x=x0+hx=x_0+h with h=x−x0h=x-x_0 admissible and 0<∣h∣<δ0<|h|<\delta, so

∣f(x)−f(x0)∣≤(∣L∣+1)∣h∣<ε.|f(x)-f(x_0)|\le(|L|+1)|h|<\varepsilon.

Hence ff is continuous at x0x_0.

Claim 2. Let ε>0\varepsilon>0. Choose δ1>0\delta_1>0 for ff and δ2>0\delta_2>0 for gg so that the respective difference quotients at x0x_0 are within ε/2\varepsilon/2 of f′(x0)f'(x_0) and of g′(x0)g'(x_0) for admissible hh with 0<∣h∣<δ10<|h|<\delta_1 (respectively δ2\delta_2). The difference quotient of f+gf+g at x0x_0 is the sum of the two difference quotients, so for admissible hh with 0<∣h∣<min⁡(δ1,δ2)0<|h|<\min(\delta_1,\delta_2),

∣(f+g)(x0+h)−(f+g)(x0)h−(f′(x0)+g′(x0))∣<ε2+ε2=ε.\Bigl|\frac{(f+g)(x_0+h)-(f+g)(x_0)}{h}-\bigl(f'(x_0)+g'(x_0)\bigr)\Bigr|<\frac{\varepsilon}{2}+\frac{\varepsilon}{2}=\varepsilon.

If ff is constant, every difference quotient equals 00, so the defining condition holds with derivative 00 for every δ\delta; in particular for c=0c=0 the function cfcf is the constant 00 and (cf)′(x0)=0=c f′(x0)(cf)'(x_0)=0=c\,f'(x_0). For c≠0c\ne0, choose δ3>0\delta_3>0 so that the difference quotient of ff is within ε/∣c∣\varepsilon/|c| of f′(x0)f'(x_0) for admissible 0<∣h∣<δ30<|h|<\delta_3; multiplying by cc shows that the difference quotient of cfcf is within ε\varepsilon of c f′(x0)c\,f'(x_0).

Claim 3. By Claim 1 applied to gg, with ε=1\varepsilon=1 in the continuity condition there is δg>0\delta_g>0 such that ∣g(x0+h)−g(x0)∣<1|g(x_0+h)-g(x_0)|<1, and hence ∣g(x0+h)∣≤K|g(x_0+h)|\le K with K=∣g(x0)∣+1≥1K=|g(x_0)|+1\ge1, for every admissible hh with ∣h∣<δg|h|<\delta_g. For admissible h≠0h\ne0, the identity

f(x0+h)g(x0+h)−f(x0)g(x0)=(f(x0+h)−f(x0))g(x0+h)+f(x0)(g(x0+h)−g(x0))f(x_0+h)g(x_0+h)-f(x_0)g(x_0)=\bigl(f(x_0+h)-f(x_0)\bigr)g(x_0+h)+f(x_0)\bigl(g(x_0+h)-g(x_0)\bigr)

gives, after dividing by hh and subtracting f′(x0)g(x0)+f(x0)g′(x0)f'(x_0)g(x_0)+f(x_0)g'(x_0),

(fg)(x0+h)−(fg)(x0)h−f′(x0)g(x0)−f(x0)g′(x0)=(f(x0+h)−f(x0)h−f′(x0))g(x0+h)+f′(x0)(g(x0+h)−g(x0))+f(x0)(g(x0+h)−g(x0)h−g′(x0)).\frac{(fg)(x_0+h)-(fg)(x_0)}{h}-f'(x_0)g(x_0)-f(x_0)g'(x_0) =\Bigl(\frac{f(x_0+h)-f(x_0)}{h}-f'(x_0)\Bigr)g(x_0+h)+f'(x_0)\bigl(g(x_0+h)-g(x_0)\bigr)+f(x_0)\Bigl(\frac{g(x_0+h)-g(x_0)}{h}-g'(x_0)\Bigr).

Let ε>0\varepsilon>0. Choose δa>0\delta_a>0 so that the difference quotient of ff is within ε/(3K)\varepsilon/(3K) of f′(x0)f'(x_0) for admissible 0<∣h∣<δa0<|h|<\delta_a; choose δb>0\delta_b>0 so that ∣g(x0+h)−g(x0)∣<ε/(3(∣f′(x0)∣+1))|g(x_0+h)-g(x_0)|<\varepsilon/\bigl(3(|f'(x_0)|+1)\bigr) for admissible ∣h∣<δb|h|<\delta_b (possible by Claim 1 applied to gg); choose δc>0\delta_c>0 so that the difference quotient of gg is within ε/(3(∣f(x0)∣+1))\varepsilon/\bigl(3(|f(x_0)|+1)\bigr) of g′(x0)g'(x_0) for admissible 0<∣h∣<δc0<|h|<\delta_c. For admissible hh with 0<∣h∣<min⁡(δg,δa,δb,δc)0<|h|<\min(\delta_g,\delta_a,\delta_b,\delta_c), the three terms on the right of the last display are bounded in absolute value by ε/3\varepsilon/3 each, so the difference quotient of fgfg is within ε\varepsilon of f′(x0)g(x0)+f(x0)g′(x0)f'(x_0)g(x_0)+f(x_0)g'(x_0). This proves the product rule.

Claim 4. Let ε>0\varepsilon>0. For φ+ψ\varphi+\psi: choose δ1,δ2>0\delta_1,\delta_2>0 with ∣φ(x)−φ(x0)∣<ε/2|\varphi(x)-\varphi(x_0)|<\varepsilon/2 for all x∈Ex\in E with ∣x−x0∣<δ1|x-x_0|<\delta_1, and ∣ψ(x)−ψ(x0)∣<ε/2|\psi(x)-\psi(x_0)|<\varepsilon/2 for all x∈Ex\in E with ∣x−x0∣<δ2|x-x_0|<\delta_2; then for x∈Ex\in E with ∣x−x0∣<min⁡(δ1,δ2)|x-x_0|<\min(\delta_1,\delta_2),

∣(φ+ψ)(x)−(φ+ψ)(x0)∣≤∣φ(x)−φ(x0)∣+∣ψ(x)−ψ(x0)∣<ε.|(\varphi+\psi)(x)-(\varphi+\psi)(x_0)|\le|\varphi(x)-\varphi(x_0)|+|\psi(x)-\psi(x_0)|<\varepsilon.

For cφc\varphi: choose δ>0\delta>0 with ∣φ(x)−φ(x0)∣<ε/(∣c∣+1)|\varphi(x)-\varphi(x_0)|<\varepsilon/(|c|+1) for x∈Ex\in E with ∣x−x0∣<δ|x-x_0|<\delta; then ∣cφ(x)−cφ(x0)∣≤∣c∣ ε/(∣c∣+1)<ε|c\varphi(x)-c\varphi(x_0)|\le|c|\,\varepsilon/(|c|+1)<\varepsilon. For φψ\varphi\psi: use the identity

φ(x)ψ(x)−φ(x0)ψ(x0)=(φ(x)−φ(x0))ψ(x)+φ(x0)(ψ(x)−ψ(x0)).\varphi(x)\psi(x)-\varphi(x_0)\psi(x_0)=\bigl(\varphi(x)-\varphi(x_0)\bigr)\psi(x)+\varphi(x_0)\bigl(\psi(x)-\psi(x_0)\bigr).

Choose δ2>0\delta_2>0 so that ∣ψ(x)−ψ(x0)∣<min⁡(1, ε2(∣φ(x0)∣+1))|\psi(x)-\psi(x_0)|<\min\Bigl(1,\ \frac{\varepsilon}{2(|\varphi(x_0)|+1)}\Bigr) for x∈Ex\in E with ∣x−x0∣<δ2|x-x_0|<\delta_2, so that also ∣ψ(x)∣≤∣ψ(x0)∣+1|\psi(x)|\le|\psi(x_0)|+1 there, and choose δ1>0\delta_1>0 so that ∣φ(x)−φ(x0)∣<ε2(∣ψ(x0)∣+1)|\varphi(x)-\varphi(x_0)|<\frac{\varepsilon}{2(|\psi(x_0)|+1)} for x∈Ex\in E with ∣x−x0∣<δ1|x-x_0|<\delta_1. For x∈Ex\in E with ∣x−x0∣<min⁡(δ1,δ2)|x-x_0|<\min(\delta_1,\delta_2), the first term is smaller than ε/2\varepsilon/2 in absolute value and the second is at most ∣φ(x0)∣⋅ε2(∣φ(x0)∣+1)<ε/2|\varphi(x_0)|\cdot\frac{\varepsilon}{2(|\varphi(x_0)|+1)}<\varepsilon/2, so ∣φ(x)ψ(x)−φ(x0)ψ(x0)∣<ε|\varphi(x)\psi(x)-\varphi(x_0)\psi(x_0)|<\varepsilon. Finally, for a constant function the difference of values at xx and x0x_0 is 00 for all x∈Ex\in E, so any δ\delta works. ■\blacksquare

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