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Dimension

Let V be a vector space with basis B . The dimension of V , denoted dim V , is the cardinality of B .

Every vector space has a basis.

Every basis for a vector space has the same cardinality.

dim V is well-defined .

If dim V , we say V is finite dimensional .

Examples

vector space field of scalars dimension
N
N
N

Every subspace is a vector space, and therefore has its own dimension.

Suppose S u 1 u k V is a linearly independent set. Then dim < S >

    Facts

  • If S is a subspace of V , then dim S dim V .
  • If dim S dim V , then S V .

Direct sums

Let V be a vector space, and let S V and T V be subspaces.

We say V is the direct sum of S and T , written V S T , if and only if for every v V , there exist unique s S and t T such that v s t .

If V S T , then T is called a complement of S .

V C { f : | f is continuous } S even funcitons in C T odd funcitons in C f t 1 2 f t f t 1 2 f t f t If f g h g h , g S and g S , h T and h T , then g g h h is odd and even, which implies g g and h h .

Facts

  • Every subspace has a complement
  • V S T if and only if
    • S T 0
    • < S , T > V
  • If V S T , and dim V , then dim V dim S dim T

Proofs

Invoke a basis.

Norms

Let V be a vector space over F . A norm is a mapping V F , denoted by , such that forall u V , v V , and F

  • u 0 if u 0
  • u u
  • u v u v

Examples

Euclidean norms:

x N : x i 1 N x i 2 1 2 x N : x i 1 N x i 2 1 2

Induced metric

Every norm induces a metric on V d u v u v which leads to a notion of "distance" between vectors.

Inner products

Let V be a vector space over F , F or . An inner product is a mapping V V F , denoted , such that

  • v v 0 , and v v 0 v 0
  • u v v u
  • a u b v w a u w b v w

Examples

N over: x y x y i 1 N x i y i

N over: x y x y i 1 N x i y i

If x x 1 x N , then x x 1 x N is called the "Hermitian," or "conjugatetranspose" of x .

Triangle inequality

If we define u u u , then u v u v Hence, every inner product induces a norm.

Cauchy-schwarz inequality

For all u V , v V , u v u v In inner product spaces, we have a notion of the angle between two vectors: u v u v u v 0 2

Orthogonality

u and v are orthogonal if u v 0 Notation: u v .

If in addition u v 1 , we say u and v are orthonormal .

In an orthogonal (orthonormal) set , each pair of vectors is orthogonal (orthonormal).

Orthogonal vectors in 2 .

Orthonormal bases

An Orthonormal basis is a basis v i such that v i v i i j 1 i j 0 i j

The standard basis for N or N

The normalized DFT basis u k 1 N 1 2 k N 2 k N N 1

Expansion coefficients

If the representation of v with respect to v i is v i a i v i then a i v i v

Gram-schmidt

Every inner product space has an orthonormal basis. Any (countable) basis can be made orthogonal by theGram-Schmidt orthogonalization process.

Orthogonal compliments

Let S V be a subspace. The orthogonal compliment S is S u u V u v 0 v v S S is easily seen to be a subspace.

If dim v , then V S S .

If dim v , then in order to have V S S we require V to be a Hilbert Space .

Linear transformations

Loosely speaking, a linear transformation is a mapping from one vector space to another that preserves vector space operations.

More precisely, let V , W be vector spaces over the same field F . A linear transformation is a mapping T : V W such that T a u b v a T u b T v for all a F , b F and u V , v V .

In this class we will be concerned with linear transformations between (real or complex) Euclidean spaces , or subspaces thereof.

Image

T w w W T v w for some v

Nullspace

Also known as the kernel: ker T v v V T v 0

Both the image and the nullspace are easily seen to be subspaces.

Rank

rank T dim T

Nullity

null T dim ker T

Rank plus nullity theorem

rank T null T dim V

Matrices

Every linear transformation T has a matrix representation . If T : 𝔼 N 𝔼 M , 𝔼 or , then T is represented by an M N matrix A a 1 1 a 1 N a M 1 a M N where a 1 i a M i T e i and e i 0 1 0 is the i th standard basis vector.

A linear transformation can be represented with respect to any bases of 𝔼 N and 𝔼 M , leading to a different A . We will always represent a linear transformation using the standard bases.

Column span

colspan A < A > A

Duality

If A : N M , then ker A A

If A : N M , then ker A A

Inverses

The linear transformation/matrix A is invertible if and only if there exists a matrix B such that A B B A I (identity).

Only square matrices can be invertible.

Let A : 𝔽 N 𝔽 N be linear, 𝔽 or . The following are equivalent:

  • A is invertible (nonsingular)
  • rank A N
  • null A 0
  • A 0
  • The columns of A form a basis.

If A A (or A in the complex case), we say A is orthogonal (or unitary ).

Questions & Answers

A golfer on a fairway is 70 m away from the green, which sits below the level of the fairway by 20 m. If the golfer hits the ball at an angle of 40° with an initial speed of 20 m/s, how close to the green does she come?
Aislinn Reply
cm
tijani
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John Reply
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Siyaka Reply
A mouse of mass 200 g falls 100 m down a vertical mine shaft and lands at the bottom with a speed of 8.0 m/s. During its fall, how much work is done on the mouse by air resistance
Jude Reply
Can you compute that for me. Ty
Jude
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emma Reply
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what is inorganic
emma
Chemistry is a branch of science that deals with the study of matter,it composition,it structure and the changes it undergoes
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Pedro
A ball is thrown straight up.it passes a 2.0m high window 7.50 m off the ground on it path up and takes 1.30 s to go past the window.what was the ball initial velocity
Krampah Reply
2. A sled plus passenger with total mass 50 kg is pulled 20 m across the snow (0.20) at constant velocity by a force directed 25° above the horizontal. Calculate (a) the work of the applied force, (b) the work of friction, and (c) the total work.
Sahid Reply
you have been hired as an espert witness in a court case involving an automobile accident. the accident involved car A of mass 1500kg which crashed into stationary car B of mass 1100kg. the driver of car A applied his brakes 15 m before he skidded and crashed into car B. after the collision, car A s
Samuel Reply
can someone explain to me, an ignorant high school student, why the trend of the graph doesn't follow the fact that the higher frequency a sound wave is, the more power it is, hence, making me think the phons output would follow this general trend?
Joseph Reply
Nevermind i just realied that the graph is the phons output for a person with normal hearing and not just the phons output of the sound waves power, I should read the entire thing next time
Joseph
Follow up question, does anyone know where I can find a graph that accuretly depicts the actual relative "power" output of sound over its frequency instead of just humans hearing
Joseph
"Generation of electrical energy from sound energy | IEEE Conference Publication | IEEE Xplore" ***ieeexplore.ieee.org/document/7150687?reload=true
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answer
Magreth
progressive wave
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Mujahid
A string is 3.00 m long with a mass of 5.00 g. The string is held taut with a tension of 500.00 N applied to the string. A pulse is sent down the string. How long does it take the pulse to travel the 3.00 m of the string?
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Source:  OpenStax, Statistical signal processing. OpenStax CNX. Jun 14, 2004 Download for free at http://cnx.org/content/col10232/1.1
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