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CS434/534: Topics in Networked (Networking) Systems Wireless Foundation: LPF; Digital Modulation and Demodulation; Wireless Channel Yang (Richard) Yang Computer Science Department Yale University 208A Watson
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Admin PS1 status
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Recap: Amplitude Modulation (AM)
Block diagram Time domain Frequency domain
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Recap: Demod of AM Design option 1: multiply modulated signal by e-jfct, and then LPF Design option 2: quadrature sampling
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Remaining Hole: How to Design LPF
Frequency domain view freq B -B freq B -B
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Recap: Design Option 1 compute freq zeroing out outband freq
compute lower-pass time signal freq B -B This is essentially how image compression works. Problem(s) of Design Option 1: FFT + IFFT
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Design Option 2: Impulse Response Filters
GNU software radio implements filtering using Finite Impulse Response (FIR) filters Infinite Impulse Response (IIR) Filters FIR filters are more commonly used FIR/IIR is essentially online, streaming algorithms They are used in networks/communications/vision/robotics…
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FIR Filter An N-th order FIR filter h is defined by an array of N+1 numbers: They are often stored backward (flipped) Assume input data stream is x0, x1, …, … hN h2 h1 h0
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xn-3 xn-2 xn-1 xn xn+1 * * * * h3 h2 h1 h0 FIR Filter compute y[n]:
3rd-Order Filter h3 h2 h1 h0 compute y[n]:
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FIR Filter xn-3 xn-2 xn-1 xn xn+1 * * * * h3 h2 h1 h0 compute y[n+1]
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FIR Filter is also called convolution between x (as a vector) and h (as a vector), denoted as
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Key Question Using h to Implement LPF
How to determine h? Approach: Understand the effects of y=g*h in the frequency domain
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g*h in the Continuous Time Domain
Remember that we consider x as samples of time domain function g(t) on [0, 1] and (repeat in other intervals) We also consider h as samples of time domain function h(t) on [0, 1] (and repeat in other intervals) for (i = 0; i< N; i++) y[t] += h[i] * g[t-i]; Ignore the 1/N part
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Visualizing g*h g(t) time h(t) T T
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Visualizing g*h g(t) g(t) time t h(0) T T
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Fourier Series of y=g*h
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In English, you can integrate
Fubini’s Theorem In English, you can integrate first along y and then along x first along x and then along y at (x, y) grid They give the same result See
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Fourier Series of y=g*h
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Summary of Progress So Far
y = g * h => Y[k] = G[k] H[k] In the case of Fourier Transform, y = g * h => Y[f] = G[f] H[f] is called the Convolution Theorem, an important theorem.
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Applying Convolution Theorem to Design LPF
Choose h() so that H() is close to a rectangle shape h() has a low order (why?) f 1/2 -1/2 1
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Sinc Function The h() is often related with the sinc(t)=sin(t)/t function f 1/2 -1/2 1
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FIR Design in Practice (Offline)
Compute h MATLAB or other design software GNU Software radio: optfir (optimal filter design) GNU Software radio: firdes (using a method called windowing method) Implement filter with given h freq_xlating_fir_filter_ccf or fir_filter_ccf
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LPF Design Example (Offline)
Design a LPF to pass signal at 1 KHz and block at 2 KHz
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LPF Design Example (Offline)
#create the channel filter # coefficients chan_taps = optfir.low_pass( 1.0, #Filter gain , #Sample Rate , #one sided mod BW (passband edge) 1800, #one sided channel BW (stopband edge) 0.1, #Passband ripple 60) #Stopband Attenuation in dB print "Channel filter taps:", len(chan_taps) #creates the channel filter with the coef found chan = gr.freq_xlating_fir_filter_ccf( 1 , # Decimation rate chan_taps, #coefficients 0, #Offset frequency - could be used to shift 48e3) #incoming sample rate
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Outline Recap Wireless background Frequency domain
Modulation and demodulation Basic concepts Amplitude modulation/demodulation Amplitude demodulation frequency shifting low pass filter and Convolution Theorem Digital modulation
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Modulation Modulation of digital signals also known as Shift Keying
Amplitude Shift Keying (ASK): vary carrier amp. according to data Frequency Shift Keying (FSK) vary carrier freq. according to bit value Phase Shift Keying (PSK) vary carrier freq. according to data 1 1 t 1 1 t 1 1 t
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Phase Shift Keying: BPSK
BPSK (Binary Phase Shift Keying): bit value 1: cosine wave cos(2πfct) bit value 0: inverted cosine wave cos(2πfct+π) very simple PSK Properties robust, used e.g. in satellite systems Q I 1 one bit time T one bit time T 1
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Phase Shift Keying: QPSK
11 01 10 00 QPSK (Quadrature Phase Shift Keying): 2 bits coded at a time we call the two bits as one symbol symbol determines shift of cosine wave often also transmission of relative, not absolute phase shift: DQPSK - Differential QPSK
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Quadrature Amplitude Modulation
Quadrature Amplitude Modulation (QAM): combines amplitude and phase modulation It is possible to code n bits using one symbol 2n discrete levels 0000 0001 0011 1000 Q I 0010 φ a Example: 16-QAM (4 bits = 1 symbol) Symbols 0011 and 0001 have the same phase φ, but different amplitude a and 1000 have same amplitude but different phase
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Generic Representation of Digital Keying (Modulation)
Sender sends symbols one-by-one M signaling functions g1(t), g2(t), …, gM(t), each has a duration of symbol time T Each value of a symbol has a signaling function
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Exercise: gi() for BPSK
1: g1(t) = cos(2πfct) t in [0, T] 0: g0(t) = -cos(2πfct) t in [0, T] Are the two signaling functions independent? Hint: think of the samples forming a vector, if it helps, in linear algebra Ans: No. g1(t) = -g0(t) Q I 1 cos(2πfct)[0, T] 1 -1 g0(t) g1(t)
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Exercise: Signaling Functions gi() for QPSK
11: cos(2πfct + π/4) t in [0, T] 10: cos(2πfct + 3π/4) t in [0, T] 00: cos(2πfct - 3π/4) t in [0, T] 01: cos(2πfct - π/4) t in [0, T] Are the four signaling functions independent? Ans: No. They are all linear combinations of sin(2πfct) and cos(2πfct). Q I 11 01 10 00 They are orthogonal because the integral of their product is 0.
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QPSK Signaling Functions as Sum of cos(2πfct), sin(2πfct)
11 00 10 11: cos(π/4 + 2πfct) t in [0, T] -> cos(π/4) cos(2πfct) + -sin(π/4) sin(2πfct) 10: cos(3π/4 + 2πfct) t in [0, T] -> cos(3π/4) cos(2πfct) + -sin(3π/4) sin(2πfct) 00: cos(- 3π/4 + 2πfct) t in [0, T] sin(3π/4) sin(2πfct) 01: cos(- π/4 + 2πfct) t in [0, T] sin(π/4) sin(2πfct) 01 [cos(3π/4), sin(3π/4)] [cos(π/4), sin(π/4)] cos(2πfct) [cos(3π/4), -sin(3π/4)] [-sin(π/4), cos(π/4)] We call sin(2πfct) and cos(2πfct) the bases.
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Outline Recap Wireless background Frequency domain
Modulation and demodulation Basic concepts Amplitude modulation/demodulation Digital modulation modulation demodulation
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Key Question: How does the Receiver Detect Which gi() is Sent?
Assume synchronized (i.e., the receiver knows the symbol boundary).
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Starting Point Considered a simple setting: sender uses a single signaling function g(), and can have two actions send g() or nothing (send 0) How does receiver use the received sequence x(t) in [0, T] to detect if sends g() or nothing?
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Design Option 1 Sample at a few time points (features) to check Issue
Not use all data points, and less robust to noise
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Design Option 2 xT x2 x1 x0 h0 h1 h2 hT *
Streaming algorithm, using all data points in [0, T] As each sample xi comes in, multiply it by a factor hT-i and accumulate to a sum y At time T, makes a decision based on the accumulated sum at time T: y[T] xT x2 x1 x0 h0 h1 h2 hT *
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Example Streaming (Convolution/Correlation):
Assume incoming x is a rectangular pulse (in baseband) and h is also a rectangular pulse A gif animation (play in ppt) presentation): redline g(): the sliding filter h(t) blue line f(): the input x() Source:
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Determining the Best h where w is noise,
Design objective: maximize peak pulse signal-to-noise ratio
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Determining the Best h Assume Gaussian noise, one can derive
Using Fourier Transform and Convolution Theorem:
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Determining the Best h Apply Schwartz inequality By considering
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Determining the Best h
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Determining Best h to Use
xT x2 x1 x0 h0 h1 h2 hT * xT x2 x1 x0 gT g2 g1 g0 *
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Matched Filter Decision
is called Matched filter. Example decision time
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Summary of Progress After this “complex” math, the implementation/interpretation is actually the following quite simple alg: precompute auto correlation: <g, g> compute the correlation between received x and signaling function g, denoted as <x, g> if <x, g> is closer to <g, g> output sends g else output sends nothing
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Applying Scheme to BPSK
Consider g1 alone, compute <x, g1>, check if close to <g1, g1>: |<x, g1> - <g1, g1>| Consider g0 alone, compute <x, g0>, check if close to <g0, g0>: |<x, g0> - <g0, g0>| Pick closer if |<x, g1> - <g1, g1>| < |<x, g0> - <g0, g0>| pick 1 else pick 0 cos(2πfct)[0, T] 1 -1 g1(t) g0(t)
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Applying Scheme to BPSK
since g0 = -g1 <x, g0> = - <x, g1> <g0, g0> = - <g0, g1> rewrite as if |<x, g1> - <g1, g1>| < |<x, g1> - <g0, g1>| pick 1 else pick 0 cos(2πfct)[0, T] 1 -1 g1(t) g0(t)
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Interpretation For any signal s, <s, g1> computes the coordinate (projection) of s when using g1 as a base cleaner if g1 is normalized (i.e., scale g1 by sqrt of <g1, g1>), but we do not worry about it yet <x, g1(t)> g1=cos(2πfct)[0, T] <g0(t), g1(t)> <g1(t), g1(t)> =-<g1(t), g1(t)>
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Applying Scheme to QPSK: Attempt 1
Consider g00 alone, compute <x, g00> … Consider g01 alone, compute <x, g01> … Consider g10 alone, compute <x, g10> … Consider g11 alone, compute <x, g11> … Issues Complexity: need to compute M correlation, where M is number of signaling functions Think of 64-QAM
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Decoding for QPSK using bases
4 signaling functions g00(), g01(), g10(), g11() For each signaling function, computes correlation with the bases (cos(), sin()), e.g., g00: [a00, b00] For received signal x, computes ax=<x, cos> and bx=<x, sin> Question: what is the meaning of a00, b00
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QPSK Demodulation/Decoding
sin(2πfct) [a00,b00] [a01,b01] [ax,bx] cos(2πfct) [a10,b10] [a11,b11] Q: how to decode?
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Look into Noise Assume sender sends gm(t) [0, T]
Receiver receives x(t) [0, T] Consider one sample where w[i] is noise Assume white noise, i.e., prob w[i] = z is
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Likelihood What is the likelihood (prob.) of observing x[i]?
it is the prob. of noise being w[i] = x[i] – g[i] What is the likelihood (prob.) of observing the whole sequence x? the product of the probabilities
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Likelihood Detection Suppose we know
Maximum likelihood detection picks the m with the highest P{x|gm}. From the expression We pick m with the lowest ||x-gm||2
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Back to QPSK Yry: Ignored noise effect: Suppose sender sends m: x(t) = g_m(t) + w(t) a_x = <g_m(t) + w(t), cos()> = a_m + <w, cos> = a_m + a_w b_x = <g_m(t) + w(t), sin()> = b_m + <w, sin> = b_m + b_w x(t) = g_m(t) + w(t) = (a_x – a_w) cos() + (b_x – b_w) sin() + n(t) = a_x cos() + b_x sin() + n’(t), where n’(t) = n(t) – a_w cos() – b_w sin() [a_x cos() + b_x sin() + n’(t) – g_i(t)]^2 = = [a_x cos() + b_x sin() – g_i(t)]^2 + n’()^2 + 2 n’()* [a_x cos() + b_x sin() – g_i(t)] Consider E[n’(t) a_x] = E[n’(t)(a_m+a_w)] = E[n’(t)a_w] =
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QPSK Demodulation/Decoding
sin(2πfct) [a00,b00] [a01,b01] [ax,bx] cos(2πfct) [a10,b10] [a11,b11] Q: what does maximum likelihood det pick?
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General Matched Filter Detection: Implementation for Multiple Sig Func.
Basic idea consider each gm[0,T] as a point (with coordinates) in a space compute the coordinate of the received signal x[0,T] check the distance between gm[0,T] and the received signal x[0,T] pick m* that gives the lowest distance value
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Computing Coordinates
Pick orthogonal bases {f1(t), f2(t), …, fN(t)} for {g1(t), g2(t), …, gM(t)} Compute the coordinate of gm[0,T] as cm = [cm1, cm2, …, cmN], where Compute the coordinate of the received signal x[0,T] as x = [x1, x2, …, xN] Compute the distance between r and cm every cm and pick m* that gives the lowest distance value
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Example: Matched Filter => Correlation Detector
received signal x
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BPSK vs QPSK fc: carrier freq. Rb: freq. of data 10dB = 10; 20dB =100
11 10 00 01
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Context Previous demodulation considers only additive noise, and does not consider wireless channel’s effects Wireless channels more than add some noise to a signaling function g(t) We next study its effects
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Outline Recap Wireless background Frequency domain
Modulation and demodulation Basic concepts Amplitude modulation/demodulation Digital modulation of additive noise channel modulation demodulation Wireless channels
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Signal Propagation
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Antennas: Isotropic Radiator
Isotropic radiator: a single point equal radiation in all directions (three dimensional) only a theoretical reference antenna Radiation pattern: measurement of radiation around an antenna z y z ideal isotropic radiator y x x Q: how does power level decrease as a function of d, the distance from the transmitter to the receiver?
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Free-Space Isotropic Signal Propagation
In free space, receiving power proportional to 1/d² (d = distance between transmitter and receiver) Suppose transmitted signal is cos(2ft), the received signal is Pr: received power Pt: transmitted power Gr, Gt: receiver and transmitter antenna gain (=c/f): wave length Sometime we write path loss in log scale: Lp = 10 log(Pt) – 10log(Pr)
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Log Scale for Large Span
dB = 10 log(times) Log Scale for Large Span ~100B 10,000 times 10,000 x 1,000 40 dB = 70 dB ~10M 1000 times 30 dB ~10K Slim/Gates Obama
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Path Loss in dB dB = 10 log(times) 40 dB 40 + 30 = 70 dB 30 dB 10 W
10,000 x 1,000 40 dB = 70 dB power 1 mW 1000 times 30 dB 1 uW source d1 d2
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dBm (Absolute Measure of Power)
dBm = 10 log (P/1mW) dBm (Absolute Measure of Power) 10 W 40 dBm 10,000 times 10,000 x 1,000 40 dB = 70 dB power 1 mW 1000 times 30 dB 1 uW -30 dBm source d1 d2
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Number in Perspective (Typical #)
Data rate (Mbps) Receive threshold (dBm) Signal/Noise (dB) 6 -82 6.02 9 -81 7.78 12 -79 9.03 18 -77 10.79 24 -74 17.04 36 -70 18.8 48 -66 24.05 54 -65 24.56
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Figure for Thought: Real Measurements
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Signal Propagation: Complexity
Receiving power additionally influenced by shadowing (e.g., through a wall or a door) refraction depending on the density of a medium reflection at large obstacles scattering at small obstacles diffraction at edges diffraction reflection refraction scattering shadow fading
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Signal Propagation: Complexity
Details of signal propagation are very complicated We want to understand the key characteristics that are important to our understanding
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Outline Recap Wireless background Frequency domain
Modulation and demodulation Basic concepts Amplitude modulation/demodulation Digital modulation of additive noise channel Wireless channels intro shadowing
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Shadowing Signal strength loss after passing through obstacles
Same distance, but different levels of shadowing: It is a random, large-scale effect depending on the environment
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Example Shadowing Effects
i.e. reduces to ¼ of signal 10 log(1/4) = -6.02
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Example Shadowing Effects
i.e. reduces to ¼ of signal 10 log(1/4) = -6.02
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Outline Recap Wireless background Frequency domain
Modulation and demodulation Basic concepts Amplitude modulation/demodulation Digital modulation of additive noise channel Wireless channels intro shadowing multipath
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Multipath Signal can take many different paths between sender and receiver due to reflection, scattering, diffraction
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Comparison Shadowing Multipath
Same distance, but different levels of shadowing by large objects It is a random, large-scale effect depending on the environment Multipath Signal of same symbol taking multiple paths may interfere constructively and destructively at the receiver also called small-scale fading
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Multipath Example: Outdoor
Example: reflection from the ground or building ground
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Multipath Effect (A Simple Example)
Assume transmitter sends out signal cos(2 fc t) d1 d2 phase difference:
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Multipath Effect (A Simple Example)
Suppose at d1-d2 the two waves totally destruct, i.e., if receiver moves to the right by /4: d1’ = d1 + /4; d2’ = d2 - /4; Discussion: how far is /4? What are implications?
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Multipath Effect (A Simple Example): Change Frequency
Suppose at f the two waves totally destruct, i.e. Smallest change to f for total construct: (d1-d2)/c is called delay spread.
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Multipath Delay Spread
RMS: root-mean-square
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Multipath Effect (moving receiver)
example d d1 d2 Suppose d1=r0+vt d2=2d-r0-vt d1d2
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Derivation See for cos(u)-cos(v)
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Derivation See for cos(u)-cos(v)
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Derivation See for cos(u)-cos(v)
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Derivation See for cos(u)-cos(v)
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Derivation See for cos(u)-cos(v)
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Derivation See for cos(u)-cos(v)
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Waveform v = 65 miles/h, fc = 1 GHz: fc v/c =
109 * 30 / 3x108 = 100 Hz 10 ms deep fade Q: how far does the car move between two deep fade?
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