Final Review Signals Flashcards
(42 cards)
Expression for an energy signal
E = integral from -infinity to +infinity (x^2(t)) dt
where does t of the energy limit tend to
0
if t in the energy limit tends to infitity, solve for
power
expression for a power signal
P = lim t->1/T * infinity of an integral from 0 to t |x^2(t)| dt
characteristic of discrete signals
has a value for only certain moments in time
characteristic of continuous signals
has a value for all moments in time
characteristic of analogue signals
has an amplitude at any time
characteristic of digital signals
finite amplitudes (square wave)
characteristic of periodic signals
signal pattern repeats for all time
characteristic of non/aperiodic signals
does not repeat
trig fourier series
an = 2/T * integral from -T/2 to T/2 (g(t)cos(nwt))dt
bn = 2/T * integral from -T/2 to T/2 (g(t)sin(nwt))dt
complex fourier series
g(t) = sum(C*e^(jnwt))
fourier transform
G(w) = integral from -infinity to infinity (g(t)e^(-jwt))dt
discrete time fourier transform
x(k) = sum(XnWn^(kn))
relationship between the coefficients of complex and trig fourier series
complex = Xn
trig = An, Bn
relationship: Xn= (An-jBn)/2
fundamental frequency equation
w = 2pi/T
T = period
If a signal can be decomposed as a linear combination of sinusoids and co-sinusoids, is it certain to result in a periodic waveform
NO
combination of sinusoinds and co-sinusoides can create nonperiodic functions
dependent of the ratio of frequencies
duality
when signals are inverses of each other
sifting theorem
if you multiply a signal by an impulse and integrate over all time, you get a signal evaluated at the time position aka. the sample of a signal
integral from -infinity to infinity(x(t)d-delta(t-Tau)dt = X(Tau) == integral from -infinity to infinity (signalimpulse) = sample
fourier transform of unit impulse
F(w) = integral from -infinity to infinity (d-delta(t)e^-jwt == 1
fourier transform of impulse train
s(t) = sum(d-delta(t-nT) = 1/T integral from -T/2to T/2 (d-delta(t)e^-jnwt dt == 1/T (e^-jnwt) evluated at t=0 === 1/T
Parsevals Theorem
integral from -infinity to infinity( |x^2(t)|)dt = 1/2pi * integral from -infinity to infinity (G^2(w)) dw
fourier transform of g(t) = x(t − τ )
time shift -> frequency shift
from reference table:
e^-jwτ G(w)
fourier transform of h(t) = x(t)* e^jωt
multiplied by a complex phasor -> modulation -> frequency shift
from reference table:
G(w-w0)