ECE101_2008FALL_EXAM1_PROFSOLN_[0]

ECE101_2008FALL_EXAM1_PROFSOLN_[0] - Midterm l ECElOl Fall...

Info iconThis preview shows pages 1–2. Sign up to view the full content.

View Full Document Right Arrow Icon
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
Background image of page 2
This is the end of the preview. Sign up to access the rest of the document.

Unformatted text preview: Midterm l ECElOl Fall 2008 Problem 1 (12 points) X(f) = 45inc(4f) X“) Problem 2 (12 points) .5 -f_c —B —f_c +B f_c —B f_c f_c +3 I m(t)cos(21rfct) Problem 3 (25 points) 0..) Y6“) l I I i ' V2, 2 ' f -(f,+ 3) -f1 0 «5l (flm) b) ;> To obtain the spectrum Z(f), we need to shift the positive half of Y(f) down by f, + B and the negative half of Y(f) up by f1+ B. This can be achieved by setting the frequency f2 of the second mixer to be :L-(fl + B). b) '9 Since film. tiplication by two cosines results in a. amplitude attenuation of 0.25, the transfer ‘ C') Theoretically, one could recover the original signal by passing the scrambled signal through the scrambler again. C x) a”, I 7,) Another acceptable answer would be to multiply z(t) by another cosine of frequency B. Low-pass filtering and amphfication by 2 would also yield the original spectrum XUl- Problem 4 (25 points) ) We’re given that = NosLd - we can find the power spectral density by a" taking Sy( f) = TlRyU m We also know that, since the phase is 0, Ho) = lH(f)le‘"g(H"” = IH me“ = |H(f)|- At this point, we’re ready to find H(f): Sn(f)|H(f)l2;Tn(f)H2(f) = Syo) = NOTTectUT) => H20”) = ———° T) = ———N°TT:,:t(fT) = 2Trect(fT) <=> H( f) = y/2Trect(fT) = x/Z—T—TecztUT) The last step comes from the fact that the rect function raised to any power simply equals the rect function. So, we’ve found H ( f), and we can now find h(t): sinc(t/T) H Trect(fT) <=> 1/Tsinc(t/T) H rect(fT) 4=> «fi/Tsincu/T) H fireaur) <=> \/—1—2—:sinc(t/T) H fireagr) 5,) Our final answer is thuslh(t) = @sincU/T). I C.) The signal y(t) is uncorrelated when = 0. Since = Nosinc(T/T), we see that condition for uncorrelation occurs whenever T = nT Where 'n. = i1, i2, :l:3... (since the sine function is O at the even and negative integers). 4,) When T increases, the autocorrelation function widens, so the signal changes more slowly. In other words, when the autocorrelation function widens it means that signal samples stay correlated for a longer time period, and so that implies slower change in the signal. Problem 5 (16 points) a.) The sampling interval is T5=111.11 usec. There are 96 channels plus I sync pulse, so the time allotted to each channel is Tc=Tsl97=l.145 usec. The pulse duration 15 1 usec, so the time between pulses is 0.145 usec. b.) / If sampled at the Nyquist rate; and the time betWeen pulses is O . 7,17,“ sgL . l v“_ V > - I V- V rs Hz ) :5 , Havana , 71- — 13/97- Luz/155‘ Problem 6 (10 points) 4.) Demodulation of standard AM is accomplished simply by using an envelope detector or square-law detector. Thus, the receivers are cheaper and less complex than those of FM systems where differentiation followed by envelope detection or zero-crossing detection must be performed. However, AM is more sensitive to amplitude distortion, Modern digital modulation techniques are more spectrally efficient than analog tech- niques. Furthermore, most information today is already in the form of bits, digital components are often cheaper and faster, and one is able to perform encryption and error correction upon digital data. ...
View Full Document

This note was uploaded on 02/27/2012 for the course CHEMISTRY/ CH/ECE/PH/ taught by Professor Faculty during the Spring '08 term at Cooper Union.

Page1 / 2

ECE101_2008FALL_EXAM1_PROFSOLN_[0] - Midterm l ECElOl Fall...

This preview shows document pages 1 - 2. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online