Partial Differentiation

Partial Differentiation

Most engineering problems involve functions with more than one independent variable (e.g., stress in a beam depending on load, length, and cross-section).

Functions of Several Variables

A function z=f(x,y)z = f(x, y) assigns a unique output zz for every pair (x,y)(x, y) in its domain. The graph of such a function is a surface in 3D space.

Partial Derivatives: The partial derivative of zz with respect to xx, denoted zx\frac{\partial z}{\partial x} or fxf_x, is found by treating yy as a constant and differentiating zz with respect to xx. Similarly, zy\frac{\partial z}{\partial y} or fyf_y treats xx as a constant.

Partial Derivatives

  1. First-Order Partial Derivatives:

    • zx=fx(x,y)\frac{\partial z}{\partial x} = f_x(x, y)
    • zy=fy(x,y)\frac{\partial z}{\partial y} = f_y(x, y)
  2. Second-Order Partial Derivatives:

    • 2zx2=fxx\frac{\partial^2 z}{\partial x^2} = f_{xx} (Differentiate w.r.t xx twice)
    • 2zy2=fyy\frac{\partial^2 z}{\partial y^2} = f_{yy} (Differentiate w.r.t yy twice)
    • 2zxy=fxy\frac{\partial^2 z}{\partial x \partial y} = f_{xy} (Differentiate w.r.t yy, then xx)
    • 2zyx=fyx\frac{\partial^2 z}{\partial y \partial x} = f_{yx} (Differentiate w.r.t xx, then yy)

    Clairaut's Theorem states that if continuous, fxy=fyxf_{xy} = f_{yx}.

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Chain Rule for Several Variables

If z=f(x,y)z = f(x, y) where xx and yy are functions of a single variable tt, then the total derivative of zz with respect to tt is:

dzdt=zxdxdt+zydydt\frac{dz}{dt} = \frac{\partial z}{\partial x}\frac{dx}{dt} + \frac{\partial z}{\partial y}\frac{dy}{dt}
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Total Differentials

The total differential dzdz approximates the change in zz due to small changes in xx (dxdx) and yy (dydy).

dz=zxdx+zydydz = \frac{\partial z}{\partial x} dx + \frac{\partial z}{\partial y} dy

This is fundamental in error analysis for experiments with multiple measured variables.