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Just because some of us can read and write and do a little math, that doesn't mean we deserve to conquer the Universe.

—Kurt Vonnegut, Hocus Pocus , 1990

This appendix gathers together all of the math facts used in the text. They are divided into six categories:

  • Trigonometric identities
  • Fourier transforms and properties
  • Energy and power
  • Z-transforms and properties
  • Integral and derivative formulas
  • Matrix algebra

So, with no motivation or interpretation, just labels, here they are:

Trigonometric identities

  • Euler's relation
    e ± j x = cos ( x ) ± j sin ( x )
  • Exponential definition of a cosine
    cos ( x ) = 1 2 e j x + e - j x
  • Exponential definition of a sine
    sin ( x ) = 1 2 j e j x - e - j x
  • Cosine squared
    cos 2 ( x ) = 1 2 1 + cos ( 2 x )
  • Sine squared
    sin 2 ( x ) = 1 2 1 - cos ( 2 x )
  • Sine and Cosine as phase shifts of each other
    sin ( x ) = cos π 2 - x = cos x - π 2 cos ( x ) = sin π 2 - x = - sin x - π 2
  • Sine–cosine product
    sin ( x ) cos ( y ) = 1 2 sin ( x - y ) + sin ( x + y )
  • Cosine–cosine product
    cos ( x ) cos ( y ) = 1 2 cos ( x - y ) + cos ( x + y )
  • Sine–sine product
    sin ( x ) sin ( y ) = 1 2 cos ( x - y ) - cos ( x + y )
  • Odd symmetry of the sine
    sin ( - x ) = - sin ( x )
  • Even symmetry of the cosine
    cos ( - x ) = cos ( x )
  • Cosine angle sum
    cos ( x ± y ) = cos ( x ) cos ( y ) sin ( x ) sin ( y )
  • Sine angle sum
    sin ( x ± y ) = sin ( x ) cos ( y ) ± cos ( x ) sin ( y )

Fourier transforms and properties

  • Definition of Fourier transform
    W ( f ) = - w ( t ) e - j 2 π f t d t
  • Definition of Inverse Fourier transform
    w ( t ) = - W ( f ) e j 2 π f t d f
  • Fourier transform of a sine
    F { A sin ( 2 π f 0 t + Φ ) } = j A 2 - e j Φ δ ( f - f 0 ) + e - j Φ δ ( f + f 0 )
  • Fourier transform of a cosine
    F { A cos ( 2 π f 0 t + Φ ) } = A 2 e j Φ δ ( f - f 0 ) + e - j Φ δ ( f + f 0 )
  • Fourier transform of impulse
    F { δ ( t ) } = 1
  • Fourier transform of rectangular pulse
  • With
    Π ( t ) = 1 - T / 2 t T / 2 0 otherwise ,
    F { Π ( t ) } = T sin ( π f T ) π f T T sinc ( f T ) .
  • Fourier transform of sinc function
    F { sinc ( 2 W t ) } = 1 2 W Π f 2 W
  • Fourier transform of raised cosine
  • With
    w ( t ) = 2 f 0 sin ( 2 π f 0 t ) 2 π f 0 t cos ( 2 π f Δ t ) 1 - ( 4 f Δ t ) 2 ,
    F { w ( t ) } = 1 | f | < f 1 1 2 1 + cos π ( | f | - f 1 ) 2 f Δ f 1 < | f | < B 0 | f | > B ,
    with the rolloff factor defined as β = f Δ / f 0 .
  • Fourier transform of square-root raised cosine (SRRC)
  • With w ( t ) given by
    1 T sin ( π ( 1 - β ) t / T ) + ( 4 β t / T ) cos ( π ( 1 + β ) t / T ) ( π t / T ) ( 1 - ( 4 β t / T ) 2 ) t 0 , ± T 4 β 1 T ( 1 - β + ( 4 β / π ) ) t = 0 β 2 T 1 + 2 π sin π 4 β + 1 - 2 π cos π 4 β t = ± T 4 β ,
    F { w ( t ) } = 1 | f | < f 1 1 2 1 + cos π ( | f | - f 1 ) 2 f Δ 1 / 2 f 1 < | f | < B 0 | f | > B .
  • Fourier transform of periodic impulse sampled signal
  • With
    F { w ( t ) } = W ( f ) ,
    and
    w s ( t ) = w ( t ) k = - δ ( t - k T s ) , F { w s ( t ) } = 1 T s n = - W ( f - ( n / T s ) ) .
  • Fourier transform of a step
  • With
    w ( t ) = A t > 0 0 t < 0 , F { w ( t ) } = A δ ( f ) 2 + 1 j 2 π f .
  • Fourier transform of ideal π / 2 phase shifter (Hilbert transformer) filterimpulse response
  • With
    w ( t ) = 1 π t t > 0 0 t < 0 , F { w ( t ) } = - j f > 0 j f < 0 .
  • Linearity property
  • With F { w i ( t ) } = W i ( f ) ,
    F { a w 1 ( t ) + b w 2 ( t ) } = a W 1 ( f ) + b W 2 ( f ) .
  • Duality property With F { w ( t ) } = W ( f ) ,
    F { W ( t ) } = w ( - f ) .
  • Cosine modulation frequency shift property
  • With F { w ( t ) } = W ( f ) ,
    F { w ( t ) cos ( 2 π f c t + θ ) } = 1 2 e j θ W ( f - f c ) + e - j θ W ( f + f c ) .
  • Exponential modulation frequency shift property
  • With F { w ( t ) } = W ( f ) ,
    F { w ( t ) e j 2 π f 0 t } = W ( f - f 0 ) .
  • Complex conjugation (symmetry) property If w ( t ) is real valued,
    W * ( f ) = W ( - f ) ,
    where the superscript * denotes complex conjugation (i.e.,  ( a + j b ) * = a - j b ) . In particular, | W ( f ) | is even and W ( f ) is odd.
  • Symmetry property for real signals Suppose w ( t ) is real.
    If w ( t ) = w ( - t ) , then W ( f ) is real. If w ( t ) = - w ( - t ) , W ( f ) is purely imaginary.
  • Time shift property
  • With F { w ( t ) } = W ( f ) ,
    F { w ( t - t 0 ) } = W ( f ) e - j 2 π f t 0 .
  • Frequency scale property
  • With F { w ( t ) } = W ( f ) ,
    F { w ( a t ) } = 1 a W ( f a ) .
  • Differentiation property
  • With F { w ( t ) } = W ( f ) ,
    d w ( t ) d t = j 2 π f W ( f ) .
  • Convolution multiplication property
  • With F { w i ( t ) } = W i ( f ) ,
    F { w 1 ( t ) * w 2 ( t ) } = W 1 ( f ) W 2 ( f )
    and
    F { w 1 ( t ) w 2 ( t ) } = W 1 ( f ) * W 2 ( f ) ,
    where the convolution operator “ * ” is defined via
    x ( α ) * y ( α ) - x ( λ ) y ( α - λ ) d λ .
  • Parseval's theorem
  • With F { w i ( t ) } = W i ( f ) ,
    - w 1 ( t ) w 2 * ( t ) d t = - W 1 ( f ) W 2 * ( f ) d f .
  • Final value theorem
  • With lim t - w ( t ) = 0 and w ( t ) bounded,
    lim t w ( t ) = lim f 0 j 2 π f W ( f ) ,
    where F { w ( t ) } = W ( f ) .

Energy and power

  • Energy of a continuous time signal s ( t ) is
    E ( s ) = - s 2 ( t ) d t
    if the integral is finite.
  • Power of a continuous time signal s ( t ) is
    P ( s ) = lim T 1 T - T / 2 T / 2 s 2 ( t ) d t
    if the limit exists.
  • Energy of a discrete time signal s [ k ] is
    E ( s ) = - s 2 [ k ]
    if the sum is finite.
  • Power of a discrete time signal s [ k ] is
    P ( s ) = lim N 1 2 N k = - N N s 2 [ k ]
    if the limit exists.
  • Power Spectral Density
  • With input and output transforms X ( f ) and Y ( f ) of a linear filter with impulse response transform H ( f ) (such that Y ( f ) = H ( f ) X ( f ) ),
    P y ( f ) = P x ( f ) | H ( f ) | 2 ,
    where the power spectral density (PSD) is defined as
    P x ( f ) = lim T | X T ( f ) | 2 T ( Watts / Hz ) ,
    where F { x T ( t ) } = X T ( f ) and
    x T ( t ) = x ( t ) Π t T ,
    where Π ( · ) is the rectangular pulse [link] .

Z-transforms and properties

  • Definition of the Z-transform
    X ( z ) = Z { x [ k ] } = k = - x [ k ] z - k
  • Time-shift property
  • With Z { x [ k ] } = X ( z ) ,
    Z { x [ k - Δ ] } = z - Δ X ( z ) .
  • Linearity property
  • With Z { x i [ k ] } = X i ( z ) ,
    Z { a x 1 [ k ] + b x 2 [ k ] } = a X 1 ( z ) + b X 2 ( z ) .
  • Final Value Theorem for z -transforms If X ( z ) converges for | z | > 1 and all poles of ( z - 1 ) X ( z ) are inside the unit circle, then
    lim k x [ k ] = lim z 1 ( z - 1 ) X ( z ) .

Integral and derivative formulas

  • Sifting property of impulse
    - w ( t ) δ ( t - t 0 ) d t = w ( t 0 )
  • Schwarz's inequality
    - a ( x ) b ( x ) d x 2 - | a ( x ) | 2 d x - | b ( x ) | 2 d x
    and equality occurs only when a ( x ) = k b * ( x ) , where superscript * indicates complex conjugation (i.e.,  ( a + j b ) * = a - j b ).
  • Leibniz's rule
    d a ( x ) b ( x ) f ( λ , x ) d λ d x = f ( b ( x ) , x ) d b ( x ) d x - f ( a ( x ) , x ) d a ( x ) d x + a ( x ) b ( x ) f ( λ , x ) x d λ
  • Chain rule of differentiation
    d w d x = d w d y d y d x
  • Derivative of a product
    d d x ( w y ) = w d y d x + y d w d x
  • Derivative of signal raised to a power
    d d x ( y n ) = n y n - 1 d y d x
  • Derivative of cosine
    d d x cos ( y ) = - ( sin ( y ) ) d y d x
  • Derivative of sine
    d d x sin ( y ) = ( cos ( y ) ) d y d x

Matrix algebra

  • Transpose transposed
    ( A T ) T = A
  • Transpose of a product
    ( A B ) T = B T A T
  • Transpose and inverse commutativity If A - 1 exists,
    A T - 1 = A - 1 T .
  • Inverse identity If A - 1 exists,
    A - 1 A = A A - 1 = I .

Questions & Answers

Three charges q_{1}=+3\mu C, q_{2}=+6\mu C and q_{3}=+8\mu C are located at (2,0)m (0,0)m and (0,3) coordinates respectively. Find the magnitude and direction acted upon q_{2} by the two other charges.Draw the correct graphical illustration of the problem above showing the direction of all forces.
Kate Reply
To solve this problem, we need to first find the net force acting on charge q_{2}. The magnitude of the force exerted by q_{1} on q_{2} is given by F=\frac{kq_{1}q_{2}}{r^{2}} where k is the Coulomb constant, q_{1} and q_{2} are the charges of the particles, and r is the distance between them.
Muhammed
What is the direction and net electric force on q_{1}= 5µC located at (0,4)r due to charges q_{2}=7mu located at (0,0)m and q_{3}=3\mu C located at (4,0)m?
Kate Reply
what is the change in momentum of a body?
Eunice Reply
what is a capacitor?
Raymond Reply
Capacitor is a separation of opposite charges using an insulator of very small dimension between them. Capacitor is used for allowing an AC (alternating current) to pass while a DC (direct current) is blocked.
Gautam
A motor travelling at 72km/m on sighting a stop sign applying the breaks such that under constant deaccelerate in the meters of 50 metres what is the magnitude of the accelerate
Maria Reply
please solve
Sharon
8m/s²
Aishat
What is Thermodynamics
Muordit
velocity can be 72 km/h in question. 72 km/h=20 m/s, v^2=2.a.x , 20^2=2.a.50, a=4 m/s^2.
Mehmet
A boat travels due east at a speed of 40meter per seconds across a river flowing due south at 30meter per seconds. what is the resultant speed of the boat
Saheed Reply
50 m/s due south east
Someone
which has a higher temperature, 1cup of boiling water or 1teapot of boiling water which can transfer more heat 1cup of boiling water or 1 teapot of boiling water explain your . answer
Ramon Reply
I believe temperature being an intensive property does not change for any amount of boiling water whereas heat being an extensive property changes with amount/size of the system.
Someone
Scratch that
Someone
temperature for any amount of water to boil at ntp is 100⁰C (it is a state function and and intensive property) and it depends both will give same amount of heat because the surface available for heat transfer is greater in case of the kettle as well as the heat stored in it but if you talk.....
Someone
about the amount of heat stored in the system then in that case since the mass of water in the kettle is greater so more energy is required to raise the temperature b/c more molecules of water are present in the kettle
Someone
definitely of physics
Haryormhidey Reply
how many start and codon
Esrael Reply
what is field
Felix Reply
physics, biology and chemistry this is my Field
ALIYU
field is a region of space under the influence of some physical properties
Collete
what is ogarnic chemistry
WISDOM Reply
determine the slope giving that 3y+ 2x-14=0
WISDOM
Another formula for Acceleration
Belty Reply
a=v/t. a=f/m a
IHUMA
innocent
Adah
pratica A on solution of hydro chloric acid,B is a solution containing 0.5000 mole ofsodium chlorid per dm³,put A in the burret and titrate 20.00 or 25.00cm³ portion of B using melting orange as the indicator. record the deside of your burret tabulate the burret reading and calculate the average volume of acid used?
Nassze Reply
how do lnternal energy measures
Esrael
Two bodies attract each other electrically. Do they both have to be charged? Answer the same question if the bodies repel one another.
JALLAH Reply
No. According to Isac Newtons law. this two bodies maybe you and the wall beside you. Attracting depends on the mass och each body and distance between them.
Dlovan
Are you really asking if two bodies have to be charged to be influenced by Coulombs Law?
Robert
like charges repel while unlike charges atttact
Raymond
What is specific heat capacity
Destiny Reply
Specific heat capacity is a measure of the amount of energy required to raise the temperature of a substance by one degree Celsius (or Kelvin). It is measured in Joules per kilogram per degree Celsius (J/kg°C).
AI-Robot
specific heat capacity is the amount of energy needed to raise the temperature of a substance by one degree Celsius or kelvin
ROKEEB
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Source:  OpenStax, Software receiver design. OpenStax CNX. Aug 13, 2013 Download for free at http://cnx.org/content/col11510/1.3
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