Differentials and Approximations

Differentials and Approximations

In engineering, exact measurements are often impossible. Differentials provide a powerful tool to approximate changes in functions and analyze error propagation.

Differentials

Let y=f(x)y = f(x) be a differentiable function. The differential dxdx is an independent variable. The differential dydy is defined as:

dy=f(x)dxdy = f'(x) dx
  • dxdx represents a small change in xx (Δx\Delta x).
  • dydy approximates the corresponding change in yy (Δy\Delta y).
  • Δydy\Delta y \approx dy for small Δx\Delta x.

Linear Approximation

We can approximate the value of a function f(x)f(x) near a known point aa using the tangent line at that point. This is called the linearization L(x)L(x) of ff at aa:

L(x)=f(a)+f(a)(xa)L(x) = f(a) + f'(a)(x - a)

For xx close to aa, f(x)L(x)f(x) \approx L(x).

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Error Propagation

If a quantity xx is measured with a possible error dxdx (or Δx\Delta x), the propagated error in a calculated quantity y=f(x)y = f(x) is approximately dydy.

  • Absolute Error: dyf(x)dxdy \approx f'(x) dx
  • Relative Error: dyyf(x)dxf(x)\frac{dy}{y} \approx \frac{f'(x) dx}{f(x)}
  • Percentage Error: Relative Error ×100%\times 100\%
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This concept is crucial in civil engineering surveying and materials testing, where measurement tolerances must be accounted for in design calculations.