MATH 414 Lecture 2

From Notes
Jump to navigation Jump to search

« previous | Wednesday, January 15, 2014 | next »


Inner Product

Most common example is the vector dot product:

u,v=uv=iuivi=|u||v|cosθ

Generalized Algebraic Structure

We induce a geometry on the algebraic definition

Length: v=v,v

Angle Between: θ=cos1(u,vuv)

The most important case is where θ=π2, in which case cosθ=0 and—more importantly—the vectors u and v are perperdicular.

Properties of the Inner Product

Positivity: u,u>0 unless u=0, in which case 0,0=0

Conjugate Symmetry: u,v=v,u. In the case of real numbers, the property becomes commutativity: u,v=v,u

Homogenuity: cu,v=cu,v

Linearity: u+w,v=u,v+w,v

Real Spaces

for n, where x=[x1xn] and y=[y1yn], we have

x,y=yTx=k=1nxkyk


Complex Spaces

for n, x,y is given by y*x (also written yHx), where y*=yH is the conjugate transpose of y.

Example: y=[i11+2i3+i], y*=[i112i3i]

Some concrete implementations of inner products may not satisfy all properties for all members of the space. [1]


Signal Spaces

Continuous and Discrete

A signal is just f(t) measured on [a,b].

Signals and Circuits

For current I(t) (essentially our function f(t))

We can measure voltage drop of a signal V(t)=RI(t)

Power at time t is given by P(t)=VI(t)=RI2(t)

Energy in time interval [a,b] is given by E=abP(t)dt=Rab|I(t)|2dt.

Hence E=ab|f(t)|2dt

Finite Energy Signals

Complex valued f(t) gives amplitude and phase.


Finite energy: ab|f(t)|2dt<. Moreover, |f(t)|2dt<

Signals don't need to be continuous (digital circuit signals) [2]

Continuous Signal Space

All signals with finite energy fit into a space:

L2={f:[a,b]ab|f(t)|2dt<}

The L comes from mathematician Lebesgue (ca. 1900), and the "square" comes from the square in the integral. The reason for this name is because integral we compute is a Lebesgue integral, not a Riemann integral. [3]

We define an inner product on L2 as

f,gL2[a,b]=abf(t)g(t)dt


Discrete Signal Space

Notation: l2

By sampling the function at fixed points, we obtain a sequence X={xn}n==(,x1,x0,x1,)

Thus l2L2.

We define our inner product by a discrete sum:

X,Yl2=n=xny¯n

The energy in a discrete signal is similarly given by

n=|xn|2


Inner Product Spaces

Schwarz's Inequality

Using axioms from definition, we arrive at

|u,v|uu, where u=u,u represents the norm of a vector uV ("LENGTH")

Triangle Inequality

Property of length:

u+vu+v.

"The sum of the lengths any two sides of a triangle must be at least the length of the third side."

Footnotes

  1. 1700s and Black Swan
  2. static pops are just discontinuities; static noise is a bunch of discontinuities in the signal
  3. A Lebesgue integral integrates over the y axis instead of the x axis. This may sound like a dumb idea, but it's brilliant because it allows us to integrate functions that would otherwise not be integrable.