Digital Integrated Circuits - Solutions for Assignment 12 | ECE 4420, Assignments of Electrical and Electronics Engineering

Material Type: Assignment; Class: Digital Integ Circuits; Subject: Electrical & Computer Engr; University: Georgia Institute of Technology-Main Campus; Term: Spring 2004;

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ECE 4420 – Spring 2004 Page 1
Homework No. 12 – Solutions
Problem 1 – P10.1
a) 0.18µm, Al, Metal 5
L=20mm, W=0.4µm, Rsq=27 m/
Rwire=Rsq×L/W
Rwire=27 m/×20mm /0.4µm=1.35 K
b) 0.13µm, Cu, Metal 8
L=20mm, W=0.4µm, Rsq=21 m/
Rwire=Rsq×L/W
Rwire=21 m/×20mm /0.4µm=1.05 K
Cint=0.1fF/µm
Cwire=Cint×L
Cwire=0.1fF/µm×20mm=2pF
τ = 0.38×Rwire×Cwire
τAl = 0.38×Rwire×Cwire= 0.38×1.35 K×2pF = 1.026 ns
τCu = 0.38×Rwire×Cwire= 0.38×1.05 K×2pF = 0.798 ns
Problem 2 – P10.3
The wire is shielded above and below so it has all the Lateral, Area and Fringing
capacitance.
T=1µm, H=0.5µm, W=0.4µm, λ=0.1µm
εox= 4εo= 4( 88.5×10-4 fF/µm) = 354×10-4 fF/µm
CLateral= εox×T/S = (354/S)×10-4 fF/µm
CArea= εox×W/H = 142×10-4 fF/µm
CFring= εox×Ln(1+T/H) = 389×10-4 fF/µm
CTotal= CLateral+CArea+CFring
S: 4λ … 40λ, Step = 4λ (0.4µm … 4µm)
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Homework No. 12 – Solutions

Problem 1 – P10.

a) 0.18μm, Al, Metal 5

L=20mm, W=0.4μm, Rsq =27 mΩ/□

Rwire =R sq ×L/W

Rwire =27 mΩ/□×20mm /0.4μm=1.35 KΩ

b) 0.13μm, Cu, Metal 8

L=20mm, W=0.4μm, Rsq =21 mΩ/□

Rwire =R sq ×L/W

Rwire =21 mΩ/□×20mm /0.4μm=1.05 KΩ

Cint =0.1fF/μm

Cwire =Cint ×L

Cwire =0.1fF/μm×20mm=2pF

τ = 0.38×Rwire ×Cwire

τAl = 0.38×R wire ×Cwire = 0.38×1.35 KΩ×2pF = 1.026 ns

τCu = 0.38×R wire ×Cwire = 0.38×1.05 KΩ×2pF = 0.798 ns

Problem 2 – P10.

The wire is shielded above and below so it has all the Lateral, Area and Fringing capacitance.

T=1μm, H=0.5μm, W=0.4μm, λ=0.1μm

εox= 4εo= 4( 88.5×

fF/μm) = 354×

fF/μm

CLateral = εox×T/S = (354/S)×

fF/μm

CArea = εox ×W/H = 142×10 -4^ fF/μm

CFring = εox ×Ln(1+T/H) = 389×10 -4^ fF/μm

CTotal= CLateral +CArea +CFring

S: 4λ … 40λ, Step = 4λ (0.4μm … 4μm)

Problem 2 - Continued

Capacitance per Spacing

Spacing

Capacitance

Problem 3 – P10.

(a) If the aggressor switches by,

then the peak value of noise on the victim line will be,

(b) Given that the aggressor net is switching in the opposite direction of the victim net, the loading capacitance on the victim net will be,

∆ V A = 1. 8 V

V

fF fF

fF V C C

C V

V

gnd C

C A V^1.^125 ( 60 100 )

C (^) L = Cgnd + 2 C (^) C = 60 fF + 2 ( 100 fF )= 260 fF