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Unformatted text preview: PRELIM 3 ECE 303 18 November 2004 NAME so/u :9 m SECTION 1. (40 points) Suppose a satellite is orbiting Jupiter. It takes light approximately 35 minutes to
travel from Jupiter to the Earth during times near closest approach. Assume that the mean
interplanetary electron density between the Earth and Jupiter is roughly 4 electrons per cc. (4 x 106
m3). The satellite transmits a series of Gaussian shaped pulses with envelopes ~ exp[(t — to)/21]2,
and with carrier frequencies of 100 MHZ and 400 MHZ. Suppose 1: = 1 microsecond (the ﬁll width
of the pulse is about 2 us) and the pulses are transmitted simultaneously at the two frequencies. (a)
What will be the difference in anival times when the pulses at the two frequencies reach the Earth?
(b) How much will the pulses at each frequency be broadened when they arrive? See the cover page for information on plasmas. Also, the formula given in class for the broadening 82 am of a Gaussian shaped pulse was r —> z": 1'[1+(—2 a 2 )2 ]“2 , where z is the distance traveled.
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interface with another semi—inﬁnite dielectric with e = 350. Suppose the incident wave is right
circularly polarized and consider two possible angles of incidence (the angle between the normal to
the interface and the direction of propagation of the incident wave), namely 35 and 45 degrees. (a)
Give the fraction of the total incident power in the reﬂected and transmitted waves for each angle of
incidence, and (b) Describe in words only (no detailed calculations needed), as completely as you
can, the polarization of the reﬂected and transmitted waves (if they exist), for each angle. 6L; \ 
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541W M (c; lyrethv, SubﬂOﬁmU’Jﬁ; ho +WSM:H‘ﬂ W 3 SW) PRELIM 3 ECE 303 18 November 2004 NAME 50/" 7'1” SECTION 3. (30 points) Suppose light in the visible spectrum (wavelengths from 400 nm to 700 nm) is
normally incident from air upon the plane surface of a semiinﬁnite dielectric with 8 = 880. We
wish to maximize the transmission (minimize the reﬂection coefﬁcient) into this dielectric by using
one or more quarter wave matching coatings of other dielectrics. However, we have only three
coating materials available to us, with a = 280, 380, and 5.380, none of which will give a perfect
“match.” What would you do and Why? Give a reason for your choice and the order and
thickness(es) of the coating(s). What fraction of the incident power would be reﬂected at the center wavelength (550 run) for your arrangement? , I
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1.636 [(30 Which to choose? The ﬁrst arrangement (1 slab) is a tiny bit better at 550 nm (but both
reﬂect only about 0.1% of the power), but we know from HW and Workshop problems
that the 2 slab scheme will work almost as well over a substantially larger wavelength
range, i.e., from 400 nm to 700 nm. So the best choice is the 2 slab arrangement shown.
Many of you used 3 slabs, giving a 1, 2, 3, 5.3, 8 sequence. This does use small steps,
which is good, but the “match” at the center is made considerably worse by adding the
380 layer. Computer calculations in Mathcad and computer plots with Matlab (see later
pages) conﬁrm this intuition. The 3 slab choice is OK, the single slab is better, and the 2
slabs (2 and 5.3) is the best. Most of you ignored the question of matching at
wavelengths other than 550 nm. Try various arrangements for QB on Prelim 3 1. What about 1, 2, 3, 5.3, 8? Thenn2~isthesameesabe¥erlautether—el=ienge 377 377 377
n 2: 377 n2 2: — n3 := —— n4 2: —— 377 it 550
2 3 5.3 8.5 2 700
where y = [39d as in Wkshp 10
Then generalize some of the above by '79 j 26,, I 3e» ( 57" 63} k 60 2. '. 1. '
Z(x1,x2,y) ;= x1  23 ;= Z(n4,n5,y)
x1  cos(y) + 1  x2  sm(y)
N23,; Z(n3,Z3,y)
"a; Z(n2,ZZ, y)
21 — 1
RM ,=<__12 2
21+“ (r1) =0.029
(lr1)2 is 0.012 for 550 nm, 0.029 for 700 nm, and 0.018 for 400 nm Pretty good, even though the "match" at the center frequency is worse than for 2 other
arrangements. (but 5e: {itsi"; 3 2. What about just one slab, with a relative dielectric constant of 3 (a 1, 3, 8
arrangement)? Then NZWIV‘: Z(n3,n5,y) (21 — n1) F12:
W 21 +n1
(lril)2=0.032 by,“ mus miss
/ 1/ 1/ Gives .000866 at 550 nm, .032 at 700 nm, .084 at 400 nm 3. Finally, what about 2 slabs, with a 1, 2, 5.3, 8 arrangement, the one I believed
would be the best? ’JngAzz Z(n4,n5,y) g3“: Z(n2,ZZ,y) r1 ::(Z1— n1)
r. M 21 + HI I
(IF1)2=2.951x 10”3 “M” ‘4' 9”” J 7cm} (WM rm”
For this 2 slab setup, (r1)2 is 0.0011 at 550 nm, 0.025 at 400 nm and 0.0030 at
700 nm 51>»: p’a'b (1491+ Faye) 46’? WW M2 (We) ECE 303 Prelim 3 #3 v/’
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.‘1; 3—25.3 500 550 600 ...
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This note was uploaded on 09/26/2007 for the course ECE 3030 taught by Professor Rana during the Fall '06 term at Cornell University (Engineering School).
 Fall '06
 RANA
 Electromagnet, Permittivity, Meier, 3 m, 3mm, circularly, ». apan

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