eifueo/docs/1b/math119.md

MATH 119: Calculus 2

Multivariable functions

!!! definition - A multivariable function accepts more than one independent variable, e.g., $f(x, y)$.

The signature of multivariable functions is indicated in the form [identifier]: [input type] → [return type]. Where $n$ is the number of inputs:

$f: \mathbb R^n \to \mathbb R$

!!! example The following function is in the form $f: \mathbb R^2\to\mathbb R$ and maps two variables into one called $z$ via function $f$.

$$(x,y)\longmapsto z=f(x,y)$$

Sketching multivariable functions

!!! definition - In a scalar field, each point in space is assigned a number. For example, topography or altitude maps are scalar fields. - A level curve is a slice of a three-dimensional graph by setting to a general variable $f(x, y)=k$. It is effectively a series of contour plots set in a three-dimensional plane. - A contour plot is a graph obtained by substituting a constant for $k$ in a level curve.

Please see level set and contour line for example images.

In order to create a sketch for a multivariable function, this site does not have enough pictures so you should watch a YouTube video.

!!! example For the function $z=x^2+y^2$:

For each $x, y, z$:

- Set $k$ equal to the variable and substitute it into the equation
- Sketch a two-dimensional graph with constant values of $k$ (e.g., $k=-2, -1, 0, 1, 2$) using the other two variables as axes

Combine the three **contour plots** in a three-dimensional plane to form the full sketch.

A hyperbola is formed when the difference between two points is constant. Where $r$ is the x-intercept:

$x^2-y^2=r^2$

If $r^2$ is negative, the hyperbola is is bounded by functions of $x$, instead.

Limits of two-variable functions

A function is continuous at $(x, y)$ if and only if all possible lines through $(x, y)$ have the same limit. Or, where $L$ is a constant:

$\text{continuous}\iff \lim_{(x, y)\to(x_0, y_0)}f(x, y) = L$

In practice, this means that if any two paths result in different limits, the limit is undefined. Substituting $x|y=0$ or $y=mx$ or $x=my$ are common solutions.

!!! example For the function $\lim_{(x, y)\to (0,0)}\frac{x^2}{x^2+y^2}$:

Along $y=0$:

$$\lim_{(x,0)\to(0, 0)} ... = 1$$

Along $x=0$:

$$\lim_{(0, y)\to(0, 0)} ... = 0$$

Therefore the limit does not exist.

Partial derivatives

Partial derivatives have multiple different symbols that all mean the same thing:

$\frac{\partial f}{\partial x}=\partial_x f=f_x$

For two-input-variable equations, setting one of the input variables to a constant will return the derivative of the slice at that constant.

By definition, the partial derivative of $f$ with respect to $x$ (in the x-direction) at point $(a, B)$ is:

$\frac{\partial f}{\partial x}(a, B)=\lim_{h\to 0}\frac{f(a+h, B)-f(a, B)}{h}$

Effectively:

• if finding $f_x$, $y$ should be treated as constant.
• if finding $f_y$, $x$ should be treated as constant.

!!! example With the function $f(x,y)=x^2\sqrt{y}+\cos\pi y$:

\begin{align*}
f_x(1,1)&=\lim_{h\to 0}\frac{f(1+h,1)-f(1,1)} h \\
\tag*{$f(1,1)=1+\cos\pi=0$}&=\lim_{h\to 0}\frac{(1+h)^2-1} h \\
&=\lim_{h\to 0}\frac{h^2+2h} h \\
&= 2 \\
\end{align*}

Higher order derivatives

!!! definition - wrt. is short for “with respect to”.

$\frac{\partial^2f}{\partial x^2}=\partial_{xx}f=f_{xx}$

Derivatives of different variables can be combined:

$f_{xy}=\frac{\partial}{\partial y}\frac{\partial f}{\partial x}=\frac{\partial^2 f}{\partial xy}$

The order of the variables matter: $f_{xy}$ is the derivative of f wrt. x and then wrt. y.

Clairaut’s theorem states that if $f_x, f_y$, and $f_{xy}$ all exist near $(a, b)$ and $f_{yx}$ is continuous at $(a,b)$, $f_{yx}(a,b)=f_{x,y}(a,b)$ and exists.

!!! warning In multivariable calculus, differentiability does not imply continuity.

Linear approximations

A tangent plane represents all possible partial derivatives at a point of a function.

For two-dimensional functions, the differential could be used to extrapolate points ahead or behind a point on a curve.

$\Delta f=f'(a)\Delta d \\ \boxed{y=f(a)+f'(a)(x-a)}$

The equations of the two unit direction vectors in $x$ and $y$ can be used to find the normal of the tangent plane:

$\vec n=\vec d_1\times\vec d_2 \\ \begin{bmatrix}-f_x(a,b) \\ -f_y(a,b) \\ 1\end{bmatrix} = \begin{bmatrix}1\\0\\f_x(a,b)\end{bmatrix} \begin{bmatrix}0\\1\\f_y(a,b)\end{bmatrix}$

Therefore, the general expression of a plane is equivalent to:

$z=C+A(x-a)+B(x-b) \\ \boxed{z=f(a,b)+f_x(a,b)(x-a)+f_y(a,b)(y-b)}$

??? tip “Proof” The general formula for a plane is $c_1(x-a)+c_2(y-b)+c_3(z-c)=0$.

If $y$ is constant such that $y=b$:

$$z=C+A(x-a)$$

which must represent in the x-direction as an equation in the form $y=b+mx$. It follows that $A=f_x(a,b)$. A similar concept exists for $f_y(a,b)$.

If both $x=a$ and $y=b$ are constant:

$$z=C$$

where $C$ must be the $z$-point.

Usually, functions can be approximated via the tangent at $x=a$.

$f(x)\simeq L(x)$

!!! warning Approximations are less accurate the stronger the curve and the farther the point is away from $f(a,b)$. A greater $|f''(a)|$ indicates a stronger curve.

!!! example Given the function $f(x,y)=\ln(\sqrt[3]{x}+\sqrt[4]{y}-1)$, $f(1.03, 0.98)$ can be linearly approximated.

$$
L(x=1.03, y=0.98)=f(1,1)=f_x(1,1)(x-1)+f_y(1,1)(y-1) \\
f(1.03,0.98)\simeq L(1.03,0.98)=0.005
$$

Differentials

Linear approximations can be used with the help of differentials. Please see MATH 117#Differentials for more information.

$\Delta f$ can be assumed to be equivalent to $df$.

$\Delta f=f_x(a,b)\Delta x+f_y(a,b)\Delta y$

Alternatively, it can be expanded in Leibniz notation in the form of a total differential:

$df=\frac{\partial f}{\partial x}dx+\frac{\partial f}{\partial y}dy$

??? tip “Proof” The general formula for a plane in three dimensions can be expressed as a tangent plane if the differential is small enough:

$$f(x,y)=f(a,b)+f_x(a,b)(x-a)+f_y(a,b)(x-b)$$

As $\Delta f=f(x,y)-f(a,b)$, $\Delta x=x-a$, and $\Delta y=y-b$, it can be assumed that $\Delta x=dx,\Delta y=dy, \Delta f\simeq df$.

$$\boxed{\Delta f\simeq df=f_x(a,b)dx+f_y(a,b)dy}$$

Related rates

Please see SL Math - Analysis and Approaches 1 for more information.

!!! example For the gas law $pV=nRT$, if $T$ increases by 1% and $V$ increases by 3%:

\begin{align*}
pV&=nRT \\
\ln p&=\ln nR + \ln T - \ln V \\
\tag{multiply both sides by $d$}\frac{d}{dp}\ln p(dp)&=0 + \frac{d}{dT}\ln T(dt)-\frac{d}{dV}\ln V(dV) \\
\frac{dp}{p} &=\frac{dT}{T}-\frac{dV}{V} \\
&=0.01-0.03 \\
&=-2\%
\end{align*}

Parametric curves

Because of the existence of the parameter $t$, these expressions have some advantages over scalar equations:

• the direction of $x$ and $y$ can be determined as $t$ increases, and
• the rate of change of $x$ and $y$ relative to $t$ as well as each other is clearer

\[ \begin{align*} f(x,y,z)&=\begin{bmatrix}x(t) \\ y(t) \\ z(t)\end{bmatrix} \\ &=(x(t), y(t), z(t)) \end{align*} \]

The derivative of a parametric function is equal to the vector sum of the derivative of its components:

$\frac{df}{dt}=\sqrt{\left(\frac{dx}{dt}\right)^2+\left(\frac{dy}{dt}\right)^2+\left(\frac{dz}{dt}\right)^2}$

Sometimes, the chain rule for multivariable functions creates a new branch in a tree for each independent variable.

For two-variable functions, if $z=f(x,y)$:

$\frac{dz}{dt}=\frac{\partial z}{\partial x}\frac{dx}{dt}+\frac{\partial z}{\partial y}\frac{dy}{dt}$

Sample tree diagram:

(Source: LibreTexts)

!!! example This can be extended for multiple functions — for the function $z=f(x,y)$, where $x=g(u,v)$ and $y=h(u,v)$:

<img src="/resources/images/many-var-tree.jpg" width=300>(Source: LibreTexts)</img>

Determining the partial derivatives with respect to $u$ or $v$ can be done by only following the branches that end with those terms.

$$
\frac{\partial z}{\partial u} = \frac{\partial z}{\partial x}\frac{\partial x}{\partial u} + \frac{\partial z}{\partial y}\frac{\partial y}{\partial u} \\
$$

!!! warning If the function only depends on one variable, $\frac{d}{dx}$ is used. Multivariable functions must use $\frac{\partial}{\partial x}$ to treat the other variables as constant.

Gradient vectors

The gradient vector is the vector of the partial derivatives of a function with respect to its independent variables. For $f(x,y)$:

$\nabla f=\left(\frac{\partial f}{\partial x},\frac{\partial f}{\partial y}\right)$

This allows for the the following replacements to appear more like single-variable calculus. Where $\vec r=(x,y)$ is a desired point, $\vec a=(a,b)$ is the initial point, and all vector multiplications are dot products:

Linear approximations are simplified to:

$f(\vec r)=f(\vec a)+\nabla f(\vec a)\bullet(\vec r-\vec a)$

The chain rule is also simplified to:

$\frac{dz}{dt}=\nabla f(\vec r(t))\bullet\vec r'(t)$

A directional derivative is any of the infinite derivatives at a certain point with the length of a unit vector. Specifically, in the unit vector direction $\vec u$ at point $\vec a=(a,b)$:

$D_{\vec u}f(a_b)=\lim_{h\to 0}\frac{f(\vec a+h\vec u)\bullet f(\vec a)}{h}$

This reduces down by taking only $h$ as variable to:

$D_{\vec u}f(a,b)=\nabla f(a,b)\bullet\vec u$

Cartesian and polar coordinates can be easily converted between:

• $x=r\sin\theta\cos\phi$
• $y=r\sin\theta\sin\phi$
• $z=r\cos\theta$

Optimisation

Local maxima / minima exist at points where all points in a disk-like area around it do not pass that point. Practically, they must have $\nabla f=0$.

Critical points are any point at which $\nabla f=0|undef$. A critical point that is not a local extrema is a saddle point.

Local maxima tend to be concave down while local minima are concave up. This can be determined via the second derivative test. For the critical point $P_0$ of $f(x,y)$:

1. Calculate $D(x,y)= f_{xx}f_{yy}-(f_{xy})^2$
2. If it greater than zero, the point is an extremum
   1. If $f_{xx}(P_0)<0$, the point is a maximum — otherwise it is a minimum
3. If it is less than zero, it is a saddle point — otherwise the test is inconclusive and you must use your eyeballs

Optimisation with constraints

If there is a limitation in optimising for $f(x,y)$ in the form $g(x,y)=K$, new critical points can be found by setting them equal to each other, where $\lambda$ is the Lagrange multiplier that determines the rate of increase of $f$ with respect to $g$:

$\nabla f = \lambda\nabla g, g(x,y)=K$

The largest/smallest values of $f(x,y)$ from the critical points return the maxima/minima. If possible, $\nabla g=\vec 0, g(x,y)=K$ should also be tested afterward.

!!! example If $A(x,y)=xy$, $g(x,y)=K: x+2y=400$, and $A(x,y)$ should be maximised:

\begin{align*}
\nabla f &= \left<y, x\right> \\
\nabla g &= \left<1, 2\right> \\
\left<y, x\right> &= \lambda \left<1, 2\right> \\
&\begin{cases}
y &= \lambda \\
x &= 2\lambda \\
x + 2y &= 400 \\
\end{cases}
\\
\\
\therefore y&=100,x=200,A=20\ 000
\end{align*}

??? example If $f(x,y)=y^2-x^2$ and the constraint $\frac{x^2}{4} + y^2=1$ must be satisfied:

\begin{align*}
\nabla f &=\left<-2x, 2y\right> \\
\nabla g &=\left<\frac{1}{2} x,2y\right> \\
\tag{$\left<0,0\right>$ does not satisfy constraints} \left<-2x,2y\right>&=\lambda\left<-\frac 1 2 x,2y\right> \\
&\begin{cases}
-2x &= \frac 1 2\lambda x \\
2y &= \lambda2y \\
\frac{x^2}{4} + y^2&= 1
\end{cases} \\
\\
2y(1-\lambda)&=0\implies y=0,\lambda=1 \\
&\begin{cases}
y=0&\implies x=\pm 2\implies\left<\pm2, 0\right> \\
\lambda=1&\implies \left<0,\pm 1\right>
\end{cases}
\\
\tag{by substitution} \max&=(2,0), (-2, 0) \\
\min&=(0, -1), (0, 1)
\end{align*}

??? example If $f(x, y)=x^2+xy+y^2$ and the constraint $x^2+y^2=4$ must be satisfied:

\begin{align*}
\tag{domain: bounded at $-2\leq x\leq 2$}y=\pm\sqrt{4-x^2} \\
f(x,\pm\sqrt{4-x^2}) &= x^2+(\pm\sqrt{4-x^2})x + 4-x^2 \\
\frac{df}{dx} &=\pm(\sqrt{4-x^2}-\frac{1}{2}\frac{1}{\sqrt{4-x^2}}2x(x)) \\
\tag{$f'(x)=0$} 0 &=4-x^2-x^2 \\
x &=\pm\sqrt{2} \\
\\
2+y^2 &= 4 \\
y &=\pm\sqrt{2} \\
\therefore f(x,y) &= 2, 6
\end{align*}

Alternatively, trigonometric substitution may be used to solve the system parametrically.

\begin{align*}
x^2+y^2&=4\implies &x=2\cos t \\
& &y=2\sin t \\
\therefore f(x,y) &= 4+2\sin(2t),0\leq t\leq 2\pi \\
\tag{include endpoints $0,2\pi$}t &= \frac\pi 4,\frac{3\pi}{4},\frac{5\pi}{4} \\
\end{align*}

!!! warning Terms cannot be directly cancelled out in case they are zero.

This applies equally to higher dimensions and constraints by adding a new term for each constraint. Given $f(x,y,z)$ with constraints $g(x,y,z)=K$ and $h(x,y,z)=M$:

$\nabla f=\lambda_1\nabla g + \lambda_2\nabla h$

Absolute extrema

• If end points exist, those should be added
• If no endpoints exist and the limits go to $\pm\infty$, there are no absolute extrema

Double integration

In a nutshell, double integration is done by taking infinitely small lines then finding the area under those lines to form a volume.

For a surface formed by vectors $[a,b]$ and $[c,d]$:

$[a,b]\times[c,d]=R=\{(x,y)|a\leq x\leq b,c\leq y\leq d\}$

If the function is continuous and bounds do not depend on variables, the order of integration doesn’t matter.

$\boxed{\int^d_c\int^b_af(x,y)dxdy}$

!!! example For $f(x,y)=x^2y$ and $R=[0,3]\times[1,2]$:

\begin{align*}
V&=\int^2_1\int^3_0x^2ydxdy \\
&=\int^2_1\left[\frac 1 3 3^3y\right]dy \\
&=\frac{9}{2}y^2\biggr|^2_1 \\
&=\frac 9 2 (4)-\frac 9 2 \\
&=\frac{27}{2}
\end{align*}

If the function is the product of two functions of separate variables, i.e., if $f(x,y)=g(x)\cdot h(y)$:

$\int^b_a\int^d_cg(x)h(y)dxdy=\left(\int^b_ah(y)dy\right)\left(\int^d_cg(x)dx\right)$

Volume betweeen two functions

The result of the bound variable should be integrated first. For functions of $y$:

$\int^b_a\left(\int^{g(x)}_{h(x)}f(x,y)dy\right)dx$

Functions can also be replaced to be bounded by the other if necessary.

!!! example For $f(x,y)$ bounded by $y=x$ and $y=\sqrt x$:

$$\int^1_0\int^{\sqrt x}_xf(x,y)dydx = \int^1_0\left(\int^y_{y^2}f(x,y)dx\right)dy$$

??? example For $f(x,y)=xy$ bounded by $x=2$, $y=0$, and $y=2x$:

\begin{align*}
\int^2_0\int^{2x}_0xy\ dydx&=\int^2_0x\left(\frac 1 2(2x)^2\right)dx \\
&=\int^2_02x^3dx \\
&=\frac 1 4 x^4(2)\biggr|^2_0 \\
&= 8
\end{align*}

Double polar integrals

The differential elements can be directly replaced:

$dA=dxdy=\rho d\rho d\phi$

In general, the radius should be the inner integral, and functions converted from Cartesian to polar forms.

$\int^{\phi_2}_{\phi_1}\int^{\rho_2}_{\rho_1}f(\rho\cos\phi,\rho\sin\phi)\rho d\rho d\phi$

Change of variables

The Jacobian is the proportion of change in the differentials between different coordinate systems.

$\frac{\partial(x,y)}{\partial(u, v)}=\det\begin{bmatrix} \partial x / \partial u & \partial x / \partial v \\ \partial y / \partial u & \partial y / \partial v \end{bmatrix}$

The Jacobian can be treated as a fraction — it may be easier to determine the reciprocal of the Jacobian and then reciprocal it again.

When converting between two systems, the absolute value of the Jacobian should be incorporated.

\[dA=\left|\frac{\partial(x,y)}{\partial(u,v)}\right|du\ dv\]

!!! example The Jacobian of the polar coordinate system relative to the Cartesian coordinate system is $\rho$. Therefore, $dA=\rho\ d\rho\ d\phi$.

If $x=x(u,v)$, $y=y(u,v)$, and $\partial(x,y)/\partial(u,v)\neq 0$ in the domain of $u$ and $v$ $D_{uv}$:

\[\iint_{D_{xy}}f(x,y)dA = \iint_{D_{uv}}f(x(u,v),y(u,v))\left|\frac{\partial(x,y)}{\partial(u,v)}\right|du\ dv\]

1. Pick a good transformation that simplifies the domain and/or the function.
2. Compute the Jacobian
3. Determine bounds (domain)
4. Integrate with the formula

If the Jacobian contains $x$ and/or $y$ terms:

• they can be substituted into the integral directly, praying that the terms all cancel out
• or $x$ and $y$ can be written in terms of $u$ and $v$ and then all substituted

!!! example For the volume within $x^2y^2\sqrt{1-x^3-y^3}$ bounded by $x=0,y=0,x^3+y^3=1$:

By graphical inspection, the bounds can be determined to be $x=0,y=0, y^3=x^3-1,x=1$.

Let $u=x^3,du=3x^2dx$. Let $v=y^3,dv=3y^2dy$. The bounds change to $0\leq u\leq 1,0\leq v\leq 1-u$.

\begin{align*}
\int^1_0\int^{1-u}_0\frac 1 9\sqrt{1-u-v}\ dudv &= \int^1_0\frac{2}{27}(1-v-u)^{3/2}\biggr|^{1-u}_0du \\
&= \int^1_0\frac{2}{27}(1-u)^{3/2}du \\
&= \frac{4}{135}(1-u)^{5/2}\biggr|^1_0 \\
&= \frac{4}{135}
\end{align*}

Applications of multiple integrals

The area enclosed within bounds $R$ is the volume with a height of 1.

$A_R=\iint_R 1\ dA$

!!! example For the area between $y=(x-1)^2$ and $y=5-(x-2)^2$:

POI: $x^2-3x=0,\therefore x=0, 3$


\begin{align*}
\int^3_0\int^{5-(x-2)^2}_{(x-1)^2}dydx &=\int^3_0(5-(x-2)^2-(x-1)^2)dx \\
&=\int^3_0(-2x^2+6x)dx \\
&=-\frac 2 3x^3+3x^2\biggr|^3_0 \\
&=9
\end{align*}

!!! example For the area of $\left(\frac x a\right)^2+\left(\frac y b\right)^2=1$ in the region $a,b>0$:

**For ellipses of this form, a direct substitution to $a\rho\cos\phi$ and $b\rho\cos\phi$ is fastest.**

Let $u=\frac x a$ and $v=\frac y b$.

$$
\frac{\partial(x,y)}{\partial(u,v)}=\det\begin{bmatrix}
a & 0 \\
0 & b
\end{bmatrix}=ab
$$

Thus $A=\iint_Rab\ du\ dv$.

Let $u=\rho\cos\phi,v=\rho\sin\phi$. Radius is 1 by inspection.

\begin{align*}
A&=\int^{2\pi}_0\int^1_0ab\rho\ d\rho\ d\phi \\
&=\int^{2\pi}\frac 1 2 ab\ d\phi \\
&=\frac 1 2 ab\phi\biggr|^{2\pi}_0 \\
&=\pi ab
\end{align*}

The average value of the function $f(x,y)$ over a region $R$, where $A_R$ is the area of the region:

$\overline{f}_R=\frac{1}{A_R}\iint_Rf(x,y) dA$

!!! example The average value of $x^2+y^2$ over $x=0,x=1, y=x$:

\begin{align*}
\text{avg}&=\frac 1 A\int^1_0\int^x_0(x^2+y^2)dydx \\
&=2\int^1_0(x^2y+\frac 1 3y^3)\biggr|^x_0dx \\
&=2\int^1_0\frac 4 3 x^3dx \\
&=\frac 2 3 x^4 \biggr|^1_0 \\
&=\frac 2 3
\end{align*}

The total “amount” of within a region, if $f(x,y)$ describes the density at point $(x,y)$:

$\iint_R f(x,y)dA$

!!! example The total of $x^2+y^2$ with density $\sigma=\sqrt{1-x^2-y^2}$:

Let $x^2=\rho\cos\phi,y^2=\rho\sin\phi$. Thus $\sigma=\sqrt{1-\rho^2}$.

\begin{align*}
M&=\int^{2\pi}_0\int^1_0\sqrt{1-\rho^2}\rho\ d\rho\ d\phi \\
&=\int^{2\pi}_0d\phi\int^1_0\sqrt{1-\rho^2}\ d\rho\ d\phi \\
\end{align*}

Let $u=1-\rho^2$. Thus $du=-2\rho\ d\rho$.

\begin{align*}
m&=2\pi\int^1_0-\frac 1 2\sqrt u du \\
&=\frac 2 3u^{3/2}du\biggr|^1_0 \\
&=\frac 2 3\pi
\end{align*}

Triple integration

Much like double integrals:

The volume within bounds $E$ is the integral of 1:

$V=\iiint_E1dV$

The average value within a volume is:

$\overline f_E=\frac 1 V\iiint_Ef(x,y,z)dV$

!!! example For the volume within $x+y+z=1$ and $2x+2y+z=2,x,y,z\geq 0$:

The points intersect the axes and each other to create the bounds $0\leq x\leq 1,0\leq y\leq 1-x,1-x-y\leq z\leq 2-2x-2y$.

$$\int^1_0\int^{1-x}_0\int^{2-2x-2y}_{1-x-y}1dz\ dy\ dx =\frac 1 6$$

The average value is:

$$6\iiint_Ez\ dV=\frac 3 4$$

The total quantity if $f$ represents density is:

$T=\iiint_Ef(x,y,z)dV$

Cylindrical coordinates

Cylindrical coordinates are effectively polar coordinates with a height.

$x=\rho\cos\phi \\ y=\rho\sin\phi \\ z=z$

$\rho=\sqrt{x^2+y^2} \\ \tan\phi=\frac y x$

The Jacobian is still $\rho$.

!!! example For the volume under $z=9-x^2-y^2$, outside $x^2+y^2=1$, and above the $xy$ plane:

- $0\leq z\leq 9-x^2-y^2\implies 0\leq z\leq 9-\rho^2$
- $1\leq \rho\leq 3$
- $0\leq \phi\leq 2\pi$

$$
\int^3_1\int^{2\pi}_0\int^{9-\rho^2}_0\rho\ dz\ d\rho\ d\phi =32\pi
$$

Spherical coordinates

Where $r$ is the direct distance from the point to the origin, $\phi$ is the angle to the x-axis in the xy-plane ($[0,2\pi]$), and $\theta$ is the angle to the z-axis, top to bottom ($[0,\pi]$):

$z=r\cos\theta \\ x=r\sin\theta\cos\phi \\ y=r\sin\theta\sin\phi$

The Jacobian is $r^2\sin\theta$.

!!! example The mass inside the sphere $x^2+y^2+z^2=9$ with density $z=\sqrt{\frac{x^2+y^2}{3}}$:

It is clear that $\tan\theta=\sqrt 3\implies\theta=\frac\pi 3,r=3$. Thus:

$$\int^3_0\int^{\pi/3}_0,\int^{2\pi}_0 \frac{\rho}{\sqrt{3}}\rho\ d\phi\ d\theta\ d\rho=\frac{243\pi}{5}$$

Approximation and interpolation

Each of these finds roots, so a rooted equation is needed.

!!! example To find an $x$ where $x=\sqrt 5$, the root of $x^2-5=0$ should be found.

Bisection

1. Select two points that are guaranteed to enclose the point
2. Select an arbitrary $x$ and check if it is greater than or less than zero
3. Slice the remaining section in half in the correct direction

Newton’s method

The below formula can be repeated after plugging in an arbitrary value.

$x_1=x_0-\frac{f(x_0)}{f'(x_0}$

!!! warning If Newton’s method converges to the wrong root, bisection is necessary to brute force the result.

Polynomial interpolation

Where $\Delta^k y_0$ are the $k$th differences between the $y$ points:

$f(x)=y_0+x\Delta y_0+x(x-1)\frac{\Delta^2y_0}{2!}+x(x-1)(x-2)\frac{\Delta^3 y_0}{3!} ...$

Taylor polynomials

The $n$th order Taylor polynomial centred at $x_0$ is:

$\boxed{P_{n,x_0}(x)=\sum^n_{k=0}\frac{f^{(k)}(x_0)(x-x_0)^k}{k!}}$

Maclaurin’s theorem states that if some function $P^{(k)}(x_0)=f^{(k)}(x_0)$ for all $k=0,...n$:

$P(x)=P_{n,x_0}(x)$

!!! example If $P(x)=1+x^3+\frac{x^6}{2}$ and \(f(x)=e^{x^5}}\), … TODO

The desired function $P(x)$ being the $n$th degree Maclaurin polynomial implies that $P(kx^m)$ is the $(mn)$th degree polynomial for $f(kx^m)$.

Therefore, if you have the Maclaurin polynomial $P(x)$ where $P$ is the $n$th order Taylor polynomial:

• $P'(x)=P_{n-1,x_0}(x)$ for $f'(x)$
• $\int P(x)dx=P_{n+1,x_0}(x)$ for $\int f(x)dx$

The integration constant $C$ can be found by substituting $x_0$ as $x$ and solving.

For $m\in\mathbb Z\geq 0$, where $P(x)$ is the Maclaurin polynomial for $f(x)$ of order $n$, $x^mP(x)$ is the $(m+n)$th order polynomial for $x^mf(x)$.

Taylor inequalities

The triangle inequality for integrals applies itself many times over the infinite sum.

$\left|\int^b_af(x)dx\right|\leq\int^b_a|f(x)|dx$

The Taylor remainder is the error between a Taylor polynomial and its actual value. Where $k$ is an arbitrary value chosen as the upper bound of the difference of the first derivative between $x_0$ and $x$: $k\geq |f^{(n+1)}(z)|$

$|R_n(x)|\leq\frac{k|x-x_0|^{n+1}}{(n+1)!}$

An approximation correct to $n$ decimal places requires that $|R_n(x)|<10^{-n}$.

!!! warning $k$ should be as small as possible. When rounding, round down for the lower bound, and round up for the upper bound.

Integral approximation

The upper and lower bounds of a Taylor polynomial are clearly $P(x)\pm R(x)$. Integrating them separately reveals creates bounds for the integral.

$\int P(x)dx-\int R(x)dx\leq\int P(x)\leq\int P(x)dx +\int R(x)dx$

Infinite series

The $n$th partial sum of a sequence is used to determine divergence.

$S_n=\sum^n_{k=0}a_k=a_0 + a_1 ... a_n$

A sum converges to $S$ if the sum eventually ends up there. Otherwise, if the limit is infinity or does not exist, it diverges.

$\lim_{x\to\infty}S_n=S\implies\sum^\infty_{n=0}a_n=S$

Divergence test

By the divergence test, if the limit of each term never reaches zero, the sum diverges.

$\lim_{x\to\infty}a_n\neq 0\implies\sum^\infty_{n=0}a_n\text{ diverges}$

Geometric series

The $n$th partial sum of a geometric series $ar^n$ is equal to:

$S_n=\frac{a(1-r)^{n+1}}{1-r}$

To simply test for convergence:

• If $|r|<1$, $S_n\to\frac{a}{1-r}$.
• Otherwise, it diverges by the test for divergence.

Integral test

If $f(x)$ is continuous, decreasing, and positive on some $[a,\infty)$:

\[\int^\infty_af(x)dx\text{ converges}\iff\sum^\infty_{k=a}f(k)\text{ converges\]

p-series test

For all $p\in\mathbb R$, a series of the form

$\sum^\infty_{n=1}\frac{1}{n^p}$

converges if and only if $p>1$.

Comparison test

For two series $\sum a_n$ and $\sum b_n$ where all terms are positive, if $a_n\leq b_n$ for all $n$, either both converge or both diverge.

The limit comparison test has the same requirements, but if $L=\lim_{n\to\infty}\frac{a_n}{b_n}$ such that $0<L<\infty$, either both converge or both diverge.

Ratio tests

The ratio test is applicable if the $L$ exists or is infinity:

$L+\lim_{n\to\infty}\left|\frac{a_{n+1}}{a_n}\right|$

• $L<1$ implies the function converges absolutely
• $L>1$ implies the function diverges
• $L=1$ is inconclusive

It is useful if a constant is raised to the power of $n$ or if a factorial is present.

The root test has the same analysis but with a different limit:

$L=\lim_{n\to\infty}\sqrt[n]{|a_n|}$

It is useful for functions of the form $f(x)^{g(x)}$.

Alternating series

If the absolute value of all terms $b_k$ continuously decreases and $\lim_{k\to b_k}=0$, the alternating function $\sum^\infty_{k=0}(-1)^kb_k$ converges.

The alternating series estimation theorem places an upper bound on the error of a partial sum. If the series passes the alternate series test, $S_n$ is the $n$th partial sum, $S$ is the sum of the series, and $b_k$ is the $k$th term:

$|S-S_n|\leq b_{n+1}$

Conditional convergence

$\sum a_n$ converges absolutely only if $\sum |a_n|$ converges.

An absolutely converging series also has its regular form converge.

A series converges conditionally if it converges but not absolutely. This indicates that it is possible for all $b\in\mathbb R$ to rearrange $\sum a_n$ to cause it to converge to $b$.

Power series

A power series centred at $x_0$ is an infinitely long polynomial.

$\sum^\infty_{n=0}c_n(x-x_0)^n$

If there are multiple identified domains of convergence, the endpoints must be tested separately to get the interval of convergence. The radius of convergence is the amplitude of the interval, regardless of inclusion/exclusion.

$r=\frac{\text{max}-\text{min}}{2}$

For a power series of radius $R$, regardless if it is differentiated, integrated, multiplied (by non-zero), the radius remains $R$.

!!! warning The interval may change.

Adding functions with different radii results in a radius roughly near the smaller interval of convergence.

The binomial series is the infinite expansion of $(1+x)^m$ with radius 1.

$(1+x)^m=\sum^\infty_{n=0}\frac{m(m-1)(m-2)...(m-n+1)}{n!}x^n$

Big O notation

A function $f$ is of order $g$ as $x\to x_0$ if $|f(x)|\leq c|g(x)|$ for all $x$ near $x_0$. This is written as big O:

$f(x)=O(g(x))\text{ as }x\to x_0$

The inner function only dictates how it grows, discarding any constant terms.

!!! example As $x\to 0$, $x^3=O(x^2)$ as well as $O(x)$ and $O(1)$. Thus $kx^3=O(x^2)$ for all $k\in\mathbb R$.

However, $x^3=O(x^4)$ only as $x\to\infty$ by the definition.

!!! example As $|\sin x|\leq |x|$, $\sin x=O(x)$ as $x\to 0$.

If $f=O(x^m)$ and $g=O(x^n)$ as $x\to 0$:

• $fg=O(x^{m+n})$
• $f+g=O(x^q)$, where q=min(m,n)
• $kO(x^n)=O(x^n)$
• $O(x^n)^m=O(x^{nm})$
• $O(x^m)\div x^n=O(x^{m-n})$

With Taylor series, big O is the remainder.

$R_n(x)=O((x-x_0)^{n+1})$

The limit of big O is the behaviour of $g(x)$.

!!! example \[\begin{align*} \lim_{x\to 0}\frac{x^2e^x+2\cos x-2}{x^3}&=\lim_{x\to 0}\frac{x^3+O(x^4)}{x^3} \\ &= 1+O(x) \\ &= 1 \end{align*}\]