Optical Communication Components and Subsystems ECE 565 Spring 2005 Homework 1 Solutions
1. Calculate the frequency and photon energy of optical communication systems operating at 0.88, 1.3 and 1.55 µm. This is best done with a short program. Solution: The frequency of a photon is related to its energy through the relation E=hν, where h is Planks constant, h=6.6262 x 10-34 Js. Also, ν = c / λ, where c is the speed of light in vacuum c = 2.9979x108 m/s, and λ is the photon’s wavelength. λ (µm )
ν (Hz)
E (J)
0.88
3.4067 x1014
0.2257 x10 18
1.4089
1.3
2.3061 x1014
0.1528 x10 18
0.9537
1.55
1.9341 x1014
0.1282 x10 18
0.7999
E (eV) -
Matlab code: h=6.6262e-34; c=2.9979e8; lambda=[0.88 1.3 1.55]*1.0e-6; nu = c ./lambda; E=h*nu; Eev = E/1.6022e-19;
2. Calculate the distances over which the optical power is attenuated by a factor of 10 for fibers with losses 0.2 dB/km and 2000 dB/km. Write a program to compute this distance for any loss quoted in dB/km. Solution: If we launch an optical power of P0 over distance L (in km), and assume that the power at the destination P, then the loss coefficient in dBm/km is α = - L-110 log10(P/P0). In this problem, P/P0 = 0.1. a=[0.2 2000]; att=0.1; L = -10 *log10(att) ./a;
L is 50 km and 5 m, for the cases of α = 0.2 dB/km and 2000 dB/km, respectively. There is a change by four orders of magnitude!
3. A single channel of an optical communication system has a bit rate of 10 Gb/s [return-tozero (RZ) format, i.e., each on-pulse is on for half of the bit duration and then it drops to zero]. In principle, how many channels can be distributed over the range 1.3 – 1.55 µm? How many in the range 1.5 – 1.6 µm?