17-Phys-B2 Electro-Optical Engineering · December 2017
Question 4 of 7: 40 km Digital Fiber Link — Dispersion and Attenuation Limits, Repeaters, Modes
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 98-Phys-B2 Electro-Optical Engineering, National
Examination December 2017 — a three-hour closed-book examination (one 8.5×11 inch
double-sided handwritten note sheet permitted). The cover page states any five of the
seven questions constitute a complete paper and only the first five as they appear in
the answer book are marked; every question is nonetheless answered in full below so the paper
remains a complete study resource. The Question 6 heading carries the
stray fragment "rework this one" — almost certainly a candidate's or marker's pencil annotation, reproduced verbatim in the question box below but not a
part of the printed exam text.
Reference texts. G. Keiser, Optical Fiber Communications, 4th ed.
(fiber modes and dispersion, link power and risetime budgets, LED/laser diode output
characteristics, PIN photodiode responsivity and noise, receiver design); B. E. A. Saleh and
M. C. Teich, Fundamentals of Photonics, 2nd ed. (semiconductor laser rate equations,
photodiode quantum efficiency and noise); A. Yariv, Quantum Electronics / E. Hecht,
Optics, 5th ed. (electro-optic modulators and Pockels cells).
Question 4: 40 km Digital Fiber Link — Dispersion and Attenuation Limits, Repeaters, Modes (20 marks)
Find. (a) dispersion-limited max repeater spacing, (b) attenuation-limited
max repeater spacing, (c) number of repeaters and link length, (d) number of guided modes.
Approach. First convert the analog signal to a bit rate (Nyquist sampling
$\times$ 9 bits/sample); the dispersion limit then compares the fiber's ray-theory intermodal
spread against half a bit period, and the attenuation limit compares the full link power budget
(laser power, minus coupling losses, margin and receiver sensitivity) against the fiber's
dB/km rating. The smaller of the two spacings sets how many repeater sections the 40 km
route needs.
Repeater layout for the 40 km route: the governing (smaller) maximum span sets the number of links needed.
Bit rate. Nyquist sampling of the 100 kHz baseband signal requires
$f_s=2B_a=200$ k samples/s; at 9 bits/sample,
$$B=f_s\times9=1.8\times10^6\ \text{bit/s}=1.8\ \text{Mb/s},\qquad T_b=\frac{1}{B}=555.6\ \text{ns}.$$
Part (a) — dispersion-limited span. The fiber's ray-theory
intermodal dispersion coefficient is
$$\frac{\Delta\tau}{L}=\frac{n_1\Delta}{c},\qquad\Delta=\frac{1.500-1.495}{1.500}=0.00333,$$
$$\frac{\Delta\tau}{L}=\frac{(1.500)(0.00333)}{2.998\times10^{8}}\times1000\ \text{m/km}
=16.68\ \text{ns/km}.$$
With the maximum allowed spread capped at half a bit period ($T_b/2=277.8$ ns), the
dispersion-limited span is
$$L_{disp}=\frac{T_b/2}{16.68\ \text{ns/km}}=\boxed{16.7\ \text{km}}.$$
Part (b) — attenuation-limited span. The receiver sensitivity
corresponding to 400 photons/bit at $\lambda=900$ nm and $B=1.8$ Mb/s is
$$P_{min}=400\,h\nu\,B=400\left(\frac{hc}{\lambda}\right)B=1.59\times10^{-10}\ \text{W}
=-68.0\ \text{dBm}.$$
The laser's 10 mW output is $+10$ dBm, so the total loss the link can tolerate
(power minus coupling losses minus margin minus receiver floor) is
$$\text{Loss}_{allowed}=10-(3+2)-5-(-68.0)=68.0\ \text{dB},$$
and dividing by the fiber's 3.5 dB/km rating,
$$L_{atten}=\frac{68.0\ \text{dB}}{3.5\ \text{dB/km}}=\boxed{19.4\ \text{km}}.$$
Part (c) — repeaters and link length. The dispersion limit
(16.7 km) is smaller than the attenuation limit (19.4 km), so the link is
dispersion-limited and no single span may exceed 16.7 km. Covering
40 km therefore needs
$$n_{links}=\left\lceil\frac{40}{16.7}\right\rceil=3\ \text{links}\ \Rightarrow\ \boxed{2\ \text{repeaters}},$$
each link being $40/3=\boxed{13.3\ \text{km}}$ long — comfortably under both the 16.7 km
and 19.4 km limits.
Part (d) — number of modes. For this fiber,
$\mathrm{NA}=\sqrt{1.500^2-1.495^2}=0.122$, and with core radius $a=50\ \mu\text{m}$ at
$\lambda=900$ nm,
$$V=\frac{2\pi a\,\mathrm{NA}}{\lambda}=\frac{2\pi(50\times10^{-6})(0.122)}{900\times10^{-9}}=42.7,$$
$$M\approx\frac{V^2}{2}=\frac{42.7^2}{2}\approx\boxed{912\ \text{modes}}.$$