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where CDcMax = maximum tolerable chromatic dispersion coefficient, s/(m m) CDMax = maximum tolerable chromatic dispersion limit, s/m = epsilon value = 03 for 1 dB power penalty and 048 for 2 dB power penalty at BER 10 12 for NRZ modulated signals z = transmission distance, m

As we said, our Web application has another content database, so we need to add elements to the XMLDocument object for that database First, we ll retrieve the additional content database using the Get-SPContentDatabase cmdlet

16 10

(80 A)2(15 )(300 s)

c 29 104 J, because all electrical energy is converted to thermal energy 25 a E Pt (022)(1000 J/s)(10 min) 1 min 13 103 J b E Pt (078)(1000 J/s)(10 min) 1 min 47 103 J 27 E IVt = I(2V)(

22

R = transmission rate, bps fc = optical carrier RMS spectral width, Hz c = speed of light in a vacuum, m/s c = carrier center wavelength, m This result estimates4 the maximum tolerable chromatic dispersion for an input Gaussian NRZ modulated optical signal at transmission distance z If the fiber link chromatic dispersion coefficient is known the result estimates the maximum transmission distance Often the laser spectral width is given as the 20 dB full width, and therefore Eq (436) can be used to convert to the RMS spectral width assuming a Gaussian spectral shape f 20dB = 6 0697 fc

(050 A)(125 V)

63 W

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060 A

11 h

115 V 12,0 00

(436)

96 10

kW)($012/kWh)

(38 A)(32 )

PS > $cd2 = Get-SPContentDatabase -WebApplication http://nimaintranet | >> Where-Object { $_Name -eq "WSS_Content2" }

(30 days)(24 h/day)

For very narrow optical sources, such as a DFB laser with a spectral width of 100 MHz, and a high transmission rate where the carrier unmodulated spectral width is f 20dB < R/10, Eq (434) is simplified to Eq (437) CD cMax z c 2 c R2

(050 A)(120 V)

858 Wh (75 A) (14 V)

060 A 2

23

R3 20 20

(437)

42 102

c No It does not depend on the resistance 5 V1 V2 IR1 IR2 IR3 V2 (3 A)(10 ) (3 A)(15 ) (3 A)(5 ) V3 30 V 30 V 45 V 15 V 45 V 15 V 90 V

53

b First, find the total resistance, then solve for voltage R V c P PA PB RA IR IV RB 255 292 547 365 V 243 W 113 W 130 W

For other optical sources where the carrier width is much wider than the modulating signal width, where f 20dB > 14R, Eq (434) is simplified to Eq (438) CD cMax z c 2 c R fc

(667 mA)(547 ) (667 mA)(365 V)

The voltage is equal across parallel resistors, so: V P1R1 P2R2 (4 W)(60 )

(667 mA)2(255 ) (667 mA)2(292 )

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d Yes The law of conservation of energy states that energy cannot be created or destroyed; therefore, the rate at which energy is converted, or power is dissipated, will equal the sum of all parts 9 The resistor with the lower resistance will dissipate less power; thus, it will be cooler

(438)

R1 22 55

R2 33

054 A

27 Then, all of the working lights are in series The 12 working lights will burn with equal intensity 22 A

120 V 55

ITU-T GSup39 epsilon values for specific optical power penalties for BER of 10 12 due to chromatic dispersion pulse spreading using NRZ modulation and DFB lasers are shown in Table 41 Using epsilon values shown in Table 41, Eq (437) can be written as Eq (439) for 1 dB power penalty Assume high bit rate transmission systems, narrow spectrum lasers (DFB), no chirp in the signal, and initial launch Gaussian NRZ pulse

24

1 a repulsive 48 V b attractive 3 the bottom (the point) 72 V 5 a from south to north b west 7 the pointed end 9 Yes Connect the potentiometer in series with the power supply and the coil Adjusting the potentiometer for more resistance will decrease the current flow and the strength of the field 17 F

1 150

R 55

Optical Power Penalty (dB) 05 1 2

Across a 33- resistor, V 120 V V2 IR2 R2 (33 )

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