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 with a scalar h and taking the limit as h→0, the definition captures the local slope along that specific direction. Using the full vector 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.
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 with a scalar h and taking the limit as h→0, the definition captures the local slope along that specific direction. Using the full vector 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.
Leibniz notation dxdy=dudydxdu resembles algebraic cancellation, but derivatives are limits, not ordinary fractions. The rigorous justification relies on expressing increments exactly as Δy=[g′(u)+ϵ]Δu with ϵ→0.
Conditions: Functions are differentiable.; The inner derivative du/dx can be zero.; The argument requires rigorous limit definitions, not informal algebra.
Leibniz notation dxdy=dudydxdu resembles algebraic cancellation, but derivatives are limits, not ordinary fractions. The rigorous justification relies on expressing increments exactly as Δy=[g′(u)+ϵ]Δu with ϵ→0.
Conditions: Functions are differentiable.; The inner derivative du/dx can be zero.; The argument requires rigorous limit definitions, not informal algebra.