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This document covers basic mathematical concepts such as linear algebra, differentiation and integration, and complex numbers. It includes definitions, notation, and standard results for each topic. The document also provides practice questions for basic skills. The linear algebra section covers matrices, vectors, linear systems, determinants, eigenvalues, and eigenvectors. The differentiation and integration section covers notation, standard results, product rule, chain rule, quotient rule, stationary points, partial derivatives, and Taylor series. The complex numbers section covers motivation, definition, complex plane, addition/subtraction, multiplication, conjugates, division, polar form, and exponential notation.
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This document contains notes on basic mathematics. There are links to the corresponding Leeds
University Library skills@Leeds page, in which there are subject notes, videos and examples.
If you require more in-depth explanations of these concepts, you can visit the Wolfram Math-
world website:
⇒ Wolfram link (http://mathworld.wolfram.com/ )
⇒ Library link
(http://library.leeds.ac.uk/tutorials/maths-solutions/pages/algebra/ ).
⇒ Library link
(http://library.leeds.ac.uk/tutorials/maths-solutions/pages/numeracy/fractions.html).
⇒ Library link
(http://library.leeds.ac.uk/tutorials/maths-solutions/pages/numeracy/indices.html).
⇒ Library link
(http://library.leeds.ac.uk/tutorials/maths-solutions/pages/mechanics/vectors.html).
⇒ Library link
(http://library.leeds.ac.uk/tutorials/maths-solutions/pages/trig geom/ ).
⇒ Library link
(http://library.leeds.ac.uk/tutorials/maths-solutions/pages/calculus/ ).
There are practice equations available online to accompany these notes.
⇒ Wolfram link (http://mathworld.wolfram.com/LinearAlgebra.html)
⇒ Library link (http://library.leeds.ac.uk/tutorials/maths-solutions/pages/mechanics/vectors.html)
2.1.1 Definitions
A matrix is a rectangular array of numbers enclosed in brackets. These numbers are called
entries or elements of the matrix.
e.g.
Matrix A has 2 rows and 3 columns.
A row vector is a matrix with a single row:
e.g. (^) [
Whereas a column vector is a matrix with a single column:
e.g.
The size of a matrix is defined by n × m where n is the number of rows and m is the number
of columns. Matrix A, as defined in equation 1, is a 2 × 3 matrix.
An element of a matrix can be described by its row position and column position. For ex-
then,
a 11 + b 11 a 12 + b 12
a 21 + b 21 a 22 + b 22
2.1.4 Subtraction
Similar to addition, corresponding elements in A and B are subtracted from each other:
a 11 − b 11 a 12 − b 12
a 21 − b 21 a 22 − b 22
2.1.5 Multiplication by a scalar
If λ is a number (i.e. a scalar) and A is a matrix, then λA is also a matrix with entries
λa 11 λa 12
λa 21 λa 22
2.1.6 Multiplication of two matrices
⇒ Wolfram link (http://mathworld.wolfram.com/MatrixMultiplication.html)
This is non-trivial and is governed by a special rule. Two matrices A , where A is of size
n × m, and B of size p × q, can only be multiplied if m = p, i.e. the number of columns in
A must match the number of rows in B. The matrix produced has size n × q, with each entry
being the dot (or scalar) product (see section 2.1.10) of a whole row in A by a whole column in
e.g. if
and^ B^ =
then
Formally, if
AB = C then
cij =
∑^ m
k=
aikbkj (9)
Aside
When using Matlab (or octave), two matrices can be multiplied in an element-wise sense. This
is NOT the same as described above.
Or we can use matrix multiplication to get all four scenarios:
2.1.8 Matrix-vector multiplication
Since a vector is a special case of a matrix, this is simply a special case of the matrix-matrix
multiplication we have already discussed. Consider multiplying a column vector of length m
by a matrix of size n × m,
e.g.
which results in a column vector of length n and in this case n = 2.
2.1.9 Special Matrices
Identity Matrix, I: The identity matrix, I, of size n × n, is defined in equation 12.
aij =
1 if i = j
0 if i 6 = j
i.e. if n = 2
This is a special case of a diagonal matrix possessing non-zero entries only on its diagonal e.g.
If A is a square n × n matrix, then the identity matrix In×n has the special property that:
NB: I is the equivalent of 1 in scalar arithmetic i.e. 1 × 2 = 2 × 1 = 2.
Transpose, A
T : If A is a n × m matrix then the transpose of A, denoted A
T , is a m × n
matrix found by swapping rows and columns of A,
e.g.
if A =
Inverse matrix, A
− 1 If A is an n×n matrix, sometimes (see later) there exists another matrix
called the inverse of A, written A
− 1 , such that
− 1 = A
− 1 A = I (15)
NB: For scalar numbers, x
− 1 is the inverse of x when considering multiplication, since
xx
− 1 = x
− 1 x = 1 (16)
⇒ Wolfram link (http://mathworld.wolfram.com/LinearSystemofEquations.html)
⇒ Video link (http://www.youtube.com/watch?v=ZK3O402wf1c)
A linear system of equations such as
5 x + 3y + z = 3
2 x − 10 y − 3 z = − 1
4 y + 5z = 7
can be written as (^)
x
y
z
as can be verified by multiplying out the left hand side. When solving the linear system Ax = b,
(where A is a matrix, x is the vector (x, y, z,... ) and b is a vector of numbers) two cases can
arise:
i) A
− 1 exists.
Then A
− 1 Ax = A
− 1 b ⇒ Ix = A
− 1 b
so x = A
− 1 b
ii) A
− 1 doesn’t exist. There is then no solution in general.
⇒ Wolfram link (http://mathworld.wolfram.com/Determinant.html)
⇒ Video link (http://www.youtube.com/watch?v=23LLB9mNJvc)
How do we know when A
− 1 exists? One method is to calculate the determinant of A, writ-
ten det A or | A |. The determinant is a single number that contains enough information about
A to determine whether it is invertible.
2 ×2 determinants: In the 2 × 2 case, if
a b
c d
then | A |= ad − bc. For example, for the linear system given by
x + 2y = 2
3 x + 4y = 3
the determinant of the coefficient matrix is
The matrix A is therefore invertible (see section 2.3.1) and so the solution exists.
As another example, consider
x + 2y = 2
2 x + 4y = 3
or (^) ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ 1 0 0
Do whichever is easier!
2.3.1 Using determinants to invert a 2 × 2 matrix
The determinant can be used in finding the inverse of a 2 × 2 matrix.
For A =
a b
c d
, the inverse can be found using the formula
detA
d −b
−c a
ad − bc
d −b
−c a
For example: find the inverse of matrix B =
− 1
3 2
1 2
⇒ Wolfram link 1 (http://mathworld.wolfram.com/Eigenvalue.html)
⇒ Wolfram link 2 (http://mathworld.wolfram.com/Eigenvector.html)
⇒ Video link (http://www.youtube.com/watch?v=lXNXrLcoerU)
Often we are interested in whether a matrix can stretch a vector. In such a case:
Av = λv , (21)
where λ is the “stretch factor”. The scalar λ is called an eigenvalue (from the German: eigen
meaning same) and v is an eigenvector. Av = λv is equivalent to:
(A − λI)v = 0. (22)
If det(A − λI) 6 = 0 then the system can be solved to find v = (A − λI)
− 1 0 = 0. If we want
non-zero vectors v, then we require |A − λI| = 0.
To find the eigenvectors and eigenvalues, we use a two stage process:
i) Solve |A − λI| = 0 ,
ii) Find v.
For example:
i) The eigenvalues λ are such that
−^ λ
For example: if λ = 4 above, then
1 1
2 2
4 4
are all eigenvectors. We typically choose the
simplest!
Matrix diagonalisation Suppose A is a n × n matrix. Form a new matrix V , each column of
which is an eigenvector of A. If V
− 1 exists then,
− 1 AV = Λ or A = V ΛV
− 1 where Λ is a diagonal matrix with (λ 1 , λ 2 ,... ),
the eigenvalues of A on the diagonal.
E.g.
then^ V^ =
NB - Eigenvector 1 is:
1 1
, eigenvector 2 is:
2 1
It turns out that V
− 1 exists and is:
Check:^ V V^
So then the matrix product
− 1 AV =
is equal to the matrix Λ.
Special case: Symmetric matrix A matrix A is symmetric if A = A
T
. It turns out that, in
this case, all the eigenvectors are orthogonal, i.e. if V 1 and V 2 are different eigenvectors, then
If each eigenvector is normalised such that Vi · Vi = 1, then,
T = V
− 1 (This is an easy way to find V
− 1 ).
Example:
T = A)
Eigenvectors λ are given by:
(1 − λ)
2 − 4 = 0
λ
2 − 2 λ − 3 = 0 or (λ − 3)(λ + 1) = 0
so, λ = 3 or λ = − 1
λ = − 1 :
x
y
⇒^ x^ +^ y^ = 0
Hence, eigenvector is:
1 − 1
But this can be normalised (since it’s magnitude is arbitrary) by any number μ : μ
1 − 1
Let’s choose μ such that: v
T v = 1, where v = μ
1 − 1
⇒ 1 = μ
2
= 2μ
2 .