M408M Learning Module Pages
Main page Chapter 10: Parametric Equations and Polar CoordinatesChapter 12: Vectors and the Geometry of SpaceChapter 13: Vector FunctionsChapter 14: Partial DerivativesLearning module LM 14.1: Functions of 2 or 3 variables:Learning module LM 14.3: Partial derivatives:Learning module LM 14.4: Tangent planes and linear approximations:Tangent planesLinearization Quadratic approximations and concavity Learning module LM 14.5: Differentiability and the chain rule:Learning module LM 14.6: Gradients and directional derivatives:Learning module LM 14.7: Local maxima and minima:Learning module LM 14.8: Absolute maxima and Lagrange multipliers:Chapter 15: Multiple Integrals |
LinearizationPartial derivatives allow us to approximate functions just like ordinary derivatives do, only with a contribution from each variable. In one dimensional calculus we tracked the tangent line to get a linearization of a function. With functions of several variables we track the tangent plane. Since the equation of the tangent plane at $(a,\, b,\, f(a, \,b))$ is $$z\ = \ f(a, b) + (x-a)f_x(a, b) + (y-b)f_y(a, b)\,,$$
Now let's use the Linearization $L(x,\, y)$ of $f$ to estimate the change $\Delta f$ in $f$ near $(a,\, b)$: $$\Delta f \ = \ f(x, y) - f(a, b)\quad \approx \quad L(x, y) - f(a, b) \quad = \quad f_x(a,b) \Delta x + f_y(a,b) \Delta y\,.$$ This is sometimes written using differentials as $$ df \ = f_x(a, b) dx + f_y(a, b) dy\,.$$ The function $L(x,\,y)$ is also called the Linear Approximation to $f$ at $(a,\,b)$.
Linearization, differentials and higher-order approximations are explained in the following video: |