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Math analysis course cheatsheet

Trigonometric functions

Angle (°)Radianssin(θ)cos(θ)tan(θ)csc(θ)sec(θ)cot(θ)
00101
30°π/61/2√3/21/√322/√3√3
45°π/4√2/2√2/21√2√21
60°π/3√3/21/2√32/√321/√3
90°π/21010
120°2π/3√3/2-1/2-√32/√3-2-1/√3
135°3π/4√2/2-√2/2-1√2-√2-1
150°5π/61/2-√3/2-1/√32-2/√3-√3
180°π0-10-1

Inverse Functions

A function has an inverse if it is bijective (one-to-one and onto). To verify that a linear function has an inverse, we ensure it is injective (one-to-one). For example,

\[f(x) = kx + b\] \[kx_1 + b = kx_2 + b\] \[kx_1 = kx_2\] \[x_1 = x_2\]

This confirms that $f(x)$ has an inverse, as it passes the injectivity test.

To find the inverse function:

\[y = kx + b\] \[x = ky + b \implies ky = x - b\] \[y = \frac{x - b}{k}\]

Thus, the inverse of $f(x)$ is:

\[f^{-1}(x) = \frac{x - b}{k}\]

Even and Odd Functions

A function is even if:

\[f(x) = f(-x)\]

Even functions are symmetric about the $y$-axis. Examples include $f(x) = x^2$ and $f(x) = \cos(x)$.

A function is odd if:

\[-f(x) = f(-x)\]

Odd functions are symmetric about the origin $(0,0)$. Examples include $f(x) = x^3$ and $f(x) = \sin(x)$.

Limits

Some important limits include:

\[\lim_{x \to 0} \frac{\sin x}{x} = 1\] \[\lim_{x \to \infty} \left(1 + \frac{k}{x}\right)^x = e^k\] \[\lim_{x \to 0} \frac{\cos x - 1}{x^2} = -\frac{1}{2}\] \[\lim_{x \to a} \frac{f(x)}{g(x)} = \lim_{x \to a} \frac{f'(x)}{g'(x)}\]

Derivatives

\[(c)' = 0\] \[(x^n)' = nx^{n-1}\] \[(\sqrt{x})' = \frac{1}{2\sqrt{x}}\] \[\left(\frac{1}{x}\right)' = -\frac{1}{x^2}\] \[(e^x)' = e^x\] \[(a^x)' = a^x \ln a\] \[(\ln x)' = \frac{1}{x}\] \[(\log_a x)' = \frac{1}{x \ln a}\] \[(\sin x)' = \cos x\] \[(\cos x)' = -\sin x\] \[(\tan x)' = \frac{1}{\cos^2 x} = \sec^2 x\] \[(\cot x)' = -\frac{1}{\sin^2 x} = -\csc^2 x\] \[(\arcsin x)' = \frac{1}{\sqrt{1 - x^2}}\] \[(\arccos x)' = -\frac{1}{\sqrt{1 - x^2}}\] \[(\arctan x)' = \frac{1}{1 + x^2}\] \[(\text{arccot} x)' = -\frac{1}{1 + x^2}\] \[(f(x)g(x))' = f'(x)g(x) + f(x)g'(x)\] \[\left( \frac{f(x)}{g(x)} \right)' = \frac{f'(x)g(x) - f(x)g'(x)}{g(x)^2}\] \[\frac{d}{dx} f(g(x)) = f'(g(x)) \cdot g'(x)\]

The derivative at point $ x_0 $ is given by:

\[f'(x_0) = \lim_{\Delta x \to 0} \frac{f(x_0 + \Delta x) - f(x_0)}{\Delta x}\]

The equation of the tangent line at the point $ (x_0, y_0) $ is:

\[y - y_0 = f'(x_0)(x - x_0)\]

The equation of the normal line (perpendicular to the tangent) is:

\[y - y_0 = -\frac{1}{f'(x_0)}(x - x_0)\]

…this can be rearranged to express $f(x)$ as follows:

\[f(x) \approx f(x_0) + f'(x_0)(x - x_0)\]

Taylor’s Theorem

Taylor’s theorem states that a function $ f(x) $ can be approximated by a polynomial $ M_n(f, x) $ near a point $ x_0 $.

Taylor Polynomial

The Taylor polynomial of degree $ n $ around the point $ x_0 $ is given by:

\[M_n(f, x) = f(x_0) + f'(x_0)(x - x_0) + \frac{f''(x_0)}{2!}(x - x_0)^2 + \cdots + \frac{f^{(n)}(x_0)}{n!}(x - x_0)^n\]

Remainder Term

The remainder term $ R_n $ quantifies the error between the actual function and the Taylor polynomial:

\[R_n(x) = \frac{f^{(n + 1)}(c)}{(n + 1)!}(x - x_0)^{n + 1}\]

where $ c $ is some point between $ x_0 $ and $ x $.

Complete Taylor Expansion

The complete Taylor expansion of $ f(x) $ around $ x_0 $ can be expressed as:

\[f(x) = M_n(f, x) + R_n(x)\]

This shows that the function can be represented as its polynomial approximation plus the error term.

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