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Answers for “导数的极限定义是什么,如何使用?”

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The directional derivative is defined as an instantaneous rate of change, requiring an infinitesimal step rather than a finite one. By scaling the direction vector v\mathbf{v} with a scalar hh and taking the limit as h→0h \to 0, the definition captures the local slope along that specific direction. Using the full vector v\mathbf{v} alone would represent a finite displacement, which fails to describe the derivative's nature as a limit of ratios over vanishingly small intervals.

Conditions: The function is differentiable at the point.; The direction is specified by a vector v.; h is a scalar approaching 0.

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Leibniz notation dydx=dydududx\frac{dy}{dx} = \frac{dy}{du}\frac{du}{dx} resembles algebraic cancellation, but derivatives are limits, not ordinary fractions. The rigorous justification relies on expressing increments exactly as Δy=[g′(u)+ϵ]Δu\Delta y = [g'(u)+\epsilon]\Delta u with ϵ→0\epsilon \to 0.

Conditions: Functions are differentiable.; The inner derivative du/dxdu/dx can be zero.; The argument requires rigorous limit definitions, not informal algebra.