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Setting up the difference quotient at x = 0

Consider the function f(x)=x2/3f(x) = x^{2/3}.

Using the limit definition of the derivative, f′(0)=lim⁡h→0f(0+h)−f(0)h,f'(0) = \lim_{h \to 0} \frac{f(0+h) - f(0)}{h}, write this limit explicitly for f(x)=x2/3f(x) = x^{2/3} and evaluate it (or determine that it does not exist). Based on your result, state whether ff is differentiable at x=0x = 0.

Hint

Substitute x=0x=0 into the difference quotient to get h2/3h\frac{h^{2/3}}{h}, simplify using exponent rules, and then examine the one-sided limits as h→0+h \to 0^+ and h→0−h \to 0^-.

Step-by-step solution

Plugging into the definition, f′(0)=lim⁡h→0h2/3−0h=lim⁡h→0h2/3hf'(0) = \lim_{h\to 0} \dfrac{h^{2/3} - 0}{h} = \lim_{h\to 0} \dfrac{h^{2/3}}{h}. Since h2/3=(h1/3)2≥0h^{2/3} = (h^{1/3})^2 \geq 0, we can simplify this as lim⁡h→0h2/3−1=lim⁡h→0h−1/3=lim⁡h→01h1/3\lim_{h\to 0} h^{2/3 - 1} = \lim_{h\to 0} h^{-1/3} = \lim_{h\to 0} \dfrac{1}{h^{1/3}}.

As h→0+h \to 0^+, h1/3→0+h^{1/3} \to 0^+, so 1h1/3→+∞\dfrac{1}{h^{1/3}} \to +\infty. As h→0−h \to 0^-, h1/3→0−h^{1/3} \to 0^-, so 1h1/3→−∞\dfrac{1}{h^{1/3}} \to -\infty. Since the two one-sided limits disagree (and neither is finite), the limit does not exist, so f′(0)f'(0) does not exist and f(x)=x2/3f(x) = x^{2/3} is not differentiable at x=0x=0 — this reflects the vertical tangent (cusp) in its graph there.

Setting up the difference quotient at x = 0 — solution graph

Interpreting the vertical tangent behavior

Near x=0x = 0, does the graph's tangent line behavior approach horizontal or vertical? Explain your reasoning based on the one-sided limits of the difference quotient from part (a).

Hint

Consider what the unbounded behavior of the difference quotient means geometrically for the slope of the tangent line.

Step-by-step solution

The tangent line behavior approaches vertical near zero. This is because the difference quotient 1h1/3\dfrac{1}{h^{1/3}} grows without bound as hh approaches zero from either side, going to positive infinity from the right and negative infinity from the left. This unbounded steepness is exactly why the limit defining the derivative fails to exist there. It reflects the sharp vertical cusp visible in the graph at that point.

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