Near a point , the tangent line to a curve is the best straight-line approximation to the curve. The linearization L(x)=f(x_0)+f'(x_0)(x-x_0) gives accurate estimates of when is close to .
| Term | Formula |
|---|---|
| Linearization | L(x)=f(x_0)+f'(x_0)(x-x_0) |
| Linear approximation | for near |
| Increment form | \Delta y\approx f'(x)\,\Delta x |
Derivation
From the definition of the derivative, for close to $0$:
\frac{f(x_0+\Delta x)-f(x_0)}{\Delta x}\approx f'(x_0)Multiplying through by :
f(x_0+\Delta x)-f(x_0)\approx f'(x_0)\,\Delta xSetting (so ):
f(x)\approx f(x_0)+f'(x_0)(x-x_0)The function
L(x)=f(x_0)+f'(x_0)(x-x_0)is called the linearization of at , and the approximation is called the linear approximation (or tangent-line approximation) of at .
Geometric interpretation: The graph of is the tangent line to at . When is close to , this tangent line stays close to the curve.

In delta notation: \Delta y\approx f'(x)\,\Delta x.
Example. For , the linear approximation at is
This says is negligible when is small (e.g., if , then ).

Worked Examples
Use the linearization of at to approximate and .
Solution
, f'(x)=\dfrac{1}{2\sqrt{x}}. , f'(9)=\dfrac{1}{6}. At : . (True value: .) At : . (True value: .)
Approximate and .
Solution
Use linearized at (since is known). f'(x)=\cos x, f'(\pi/6)=\cos(\pi/6)=\sqrt{3}/2. Since rad: (True values: $0.5150$ and $0.4848$, respectively.)
What is the linear approximation of at ? For what values of is it accurate to within $0.01$?
Solution
, f'(0)=1. The linearization is . This famous approximation holds for small (in radians). For accuracy within $0.01$: we need . From the graph of , this holds when (approximately ).
When Is Linear Approximation Accurate?
The linear approximation is accurate when the curve has little "bending" near . A sharp bend at means the tangent line quickly diverges from the curve.

The "bending" of a curve is measured by the second derivative (covered in Chapter 4).
Application: The Pendulum
A simple pendulum of length and mass satisfies:
This nonlinear equation has no closed-form solution in terms of elementary functions. Using the linear approximation (valid for small angles), we replace it by:
whose solution is
This approximation is valid for .
