The Entirety of Mathematics in Two Hours
“Do not worry about your problems with mathematics, I assure you mine are far greater”
- Albert Einstein Some Simple Functions: Polynomials
y=x
Some Simple Functions: Polynomials
Some Simple Functions: Polynomials
Simultaneous Equations
Here we have two equations and require they are both true simultaneously.
Function Notation
To show that y depends on x we write:
The name The variable it of the function depends on
If a function depends on more variables we write
Some Simple Functions: Trigonometic
c b
a
Some Simple Functions: Trigonometic
Degrees vs Radians
360 degrees = 2π radians
Degrees:
θ
Radians:
Everything is just a little bit simpler with radians Some Simple Functions: Trigonometic
Some Simple Functions: Exponential
Defining Functions
● sin, cos and exp difficult to evaluate
● Polynomials easy to evaluate
● Define special functions in terms of a polynomial 'expansion'
Approximating sin
Approximating sin
Approximating sin
Approximating sin
Defining Special Functions
Summation Notation
We call this a series – a list of numbers added together
The fourth term The first term The third term The second term
In this case, the term and there are 4 terms.
Summation Notation
What we are We write summing to
The general term
What we are Index we are summing from summing over
“Sum `n' from 1 to 4”
Summation Notation
The `form' of the general term is clearly
So,
Summation Notation
Complex Numbers
Square roots of positive numbers are well defined:
or
or
But what about negative numbers?
?
Complex Numbers
Let us invent a new number:
Note: this is sometimes called j
Complex Numbers
We can now find the square root of any negative number:
Complex Numbers
We move from a number line to a number plane:
An Argand Diagram. Complex Numbers
- real part
- imaginary part
Complex Numbers
Complex Numbers
Complex Numbers
We have the remarkable result that:
This is Euler's Formula
The exponential function is closely linked to the trigonometric functions
Leonard Euler
● Functional analysis ● Mechanics ● Fluid Dynamics ● Astronomy ● Optics ● ...
Matrices and Vectors
We can list (numeric) information as a vector
- a row vector
- a column vector
We denote a vector as v or v e.g.
Matrices and Vectors
We can also store information in a matrix
Or more generically,
Matrices and Vectors
We can multiply vectors and matrices.
We multiply each row of the matrix by the vector in turn
Matrices and Vectors
Matrices and Vectors
Another example:
This is the Identity Matrix, denoted I. Matrices and Vectors
In general,
Matrices and Vectors
Generalising even further, we have
which have elements , and .
And we have the formula:
Matrices and Vectors
We can write simultaneous equations in this form:
is equivalent to
or more generically
Matrices and Vectors
If we have matrix A, we define its inverse, A-1, as
We can then rewrite the system of equations:
So we can thus calculate x
Calculus
Isaac Newton Gottfried Wilhelm von Leibniz Calculus
Denounced by Bishop George Berkeley in `The Analyst: A discourse addressed to an infidel mathematician' Described calculus as `the ghosts of departed quantities'
Given a firmer footing by Cauchy and Weierstrass Berkeley
Differentiation
How does a function y vary with x? ie, given a change in x of Δx what is Δy, the corresponding change in y?
Differentiation
For a straight line:
The gradient is Differentiation
A curve can be approximated with a series of lines, each of length
The shorter the lines, the more accurate approximation. It becomes precise as
Straight Line Approximation
We can approximate a circle with a series of straight-sided polygons
4 sides 5 6 8
12 20
Differentiation
Differentiating
Differentiation
Differentiating
So, Differentiation
Integration
What is the area under a curve?
` `
The narrower the rectangles, the more accurate approximation. It becomes precise as Integration
Integration
The Fundamental Theorem of Calculus
For any function: Let us define another funtion, , such that
is the integral of
The Fundamental Theorem of Calculus
Then, we have the relation:
Integration and differentiation are the opposite of each other!
Example of Calculus distance, x
time, t
How fast distance changes (with time) is speed.
Example of Calculus
speed, v
time, t
distance = speed x time = area under the graph
Calculus Notation
A Violin String
A Violin String
Generally one doesn't here a single mode
A superposition of modes occurs instead This adds to the `texture' of the sound
Combinations of modes are simply added
A Violin String
Mode 1
Mode 2
Mode 1 + Mode 2
A Violin String
Fourier Series
By adding together and
Josef Fourier in various ratios we can approximate any* function by it's Fourier Series.
*well, almost any
Fourier Series
For example,
Fourier Series
A Fourier Series is always periodic, so must repeat every 2π
Fourier Series
The general form of a Fourier series is
But how do we find the coefficients and ?
Fourier Series
There is another form of the Fourier series...
where
Fourier Transforms (kind of)
Vibration-o-metre
Plate
Piston
What is driving the plate?
Fourier Transforms (kind of)
Create a Fourier Series for the `time signal', .
We find that all the coefficients are 0, except for:
So the three pistons are vibrating with frequencies
1 4 10 Differential Equations
Population Growth: Number of babies is proportional to number of adults
provides the time scale – a small value gives a small growth rate
We also require an initial condition,
Differential Equations
time
Differential Equations
● Exponential growth reasonable if there is no limitation on resources: eg Bacteria in a petri dish
● If resources are limited, we expect there to be a reduction in growth as we approach a limiting maximum population.
Differential Equations
The logistic equation:
It is nonlinear
Differential Equations
So, for small P we have unrestrained growth but for larger P it is restricted Differential Equations
Levels off near max value
Exponential Growth
time
Differential Equations
Overpopulation
Levels off near max value
time
Differential Equations
● This is an ordinary differential equation – ODE We have only one dependent variable (P) and one independent variable (t)
● What if our function depended on two variables? eg time and location
● We will create a partial differential equation - PDE
Multivariable Calculus
For a function of one variable, we ask how does y(x) vary with respect to x
For a function of two variables, we ask how does y(x,t) vary with respect to either x or t.
So, conceptually it is just the same
Differential Equations The Heat Equation
- the internal heat density
- the heat flux
Change in total heat = difference in flux
Differential Equations The Heat Equation
- the internal heat density
- the heat flux
A conservation law
Differential Equations The Heat Equation ● Fick's Law: The flux of heat is proportional to the temperature gradient
ie
So,
Adolf Fick The Heat Equation Differential Equations
Differential equations must be solved subject to given conditions. eg the population equation required an initial condition
Generally, if you have a time derivative you need a temporal condition. If you have a spatial derivative you need a spatial condition. eg we solve the heat equation subject to the initial condition
and boundary condition
Differential Equations
We put a cake in the oven:
The cake has an initial temperature - the initial condition The oven is a constant temperature - the boundary condition
Differential Equations
The conditions are just as important as the equation itself
e.g. For the logistic equation, and exhibit completely different behaviour.
Likewise a glass of water put in the freezer and a glass of water put in the oven obey the same equation but behave completely differently.