ECE Department, University of Illinois ECE 552 Numerical Circuit Analysis I. Hajj Spring 2015...
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Transcript of ECE Department, University of Illinois ECE 552 Numerical Circuit Analysis I. Hajj Spring 2015...
ECE Department, University of IllinoisECE 552
Numerical Circuit Analysis
I. HajjSpring 2015
Lecture One
INTRODUCTION
Copyright © I. Hajj 2012 All rights reserved
Introduction
• System analysis is a basic step in system design
• Computer-Aided analysis or simulation helps in the design of complex systems before the systems are built or manufactured
Four steps of system simulation
1. System modeling, including component and device modeling
2. System equation formulation
3. Equation solution
4. Display and interpretation of solution
Assumption
To start, we consider Electric Circuits that are modeled as interconnections of lumped elements (as opposed to distributed elements): Resistors; capacitors; inductors; independent sources.
We will not consider the derivation of device models in this course. We will assume that device models are provided. We will concentrate on equation formulation and equation solution techniques.
Circuit equations include two components:
• Element characteristics
• Topological equations or how the elements are interconnected
Types of Equations to be Solved
• Linear equations
• Nonlinear algebraic equations
• Differential-algebraic equations
• Partial differential equations (distributed elements)
Element Characteristics(Chapter 1)
Resistors
• Characterized by an algebraic relation between voltage v and current i
(Note the associated reference directions of v and i)
Linear two-terminal resistor (Ohm's Law)
v = ri
i = gv
r, g are constant => time-invariant r(t), g(t) => time-varying
Independent Sources
Voltage Sources Examples: v = 5 V, v = B cos(ωt + Φ) V
Remark: Independent sources are characterized by an algebraic relationship
Linear Multiterminal Resistors
i = [G]v, v = [R]i
or
If G, R, or H are constant matrices, then resistor is time-invariant; if they are functions of time, then resistor is time-variant.
"Controlled" or "Dependent" sources, e.g., il=αv2, v2=βvl
can be considered as part of a two-port representation
Example
General form of linear resistorcharacteristics, including dependent and independent sources is:
[G]v + [R]i = s
Circuit Diagram
3-Terminal
Remark: Terminal equations are sufficient. There is no need to represent multiterminal or multiport as interconnection of 2-Terminal elements (see above)
2-Port
Macromodeling (e.g. , Op-Amp)
Resistive macromodel
• Relation between voltages and currents at terminals or ports are derived from the internal equations.
• Internal voltages and currents of macromodel can be computed later, if desired. This leads the Hierarchical Analysis.
Nonlinear Resistors
Two terminals
i = g(v)
voltage-controlled
v
v
i
v
f(i,v) = 0
v = r(i)
current-controlled
v
Linear, time-invariant
Time-varying linear capacitor
In steady-state sinusoidal analysis
Ic = ( jωC ) Vc
Capacitors
Multiterminal Inductor
∅𝑳 = 𝑳 𝒊𝑳 (linear) ∅𝑳 = f (𝒊𝑳) (nonlinear) 𝒗𝑳 = 𝒅∅𝑳𝒅𝒕
∅𝑳 , 𝒊𝑳 , 𝒗𝑳 are vectors
L is a matrix
Linear Two-Port Inductor (Transformer)
𝒊𝟏 𝒊𝟐
+ • • +
𝒗𝟏 ∅𝟏 ∅𝟐 𝒗𝟐
_ _
ቈ∅𝟏∅𝟐 = 𝑳𝟏 𝑴
𝑴 𝑳𝟐൩ ቈ𝒊𝟏𝒊𝟐
𝒗𝟏𝒗𝟐൩ = 𝑳𝟏 𝑴
𝑴 𝑳𝟐൩ ൦𝒅𝒊𝟏𝒅𝒕𝒅𝒊𝟐𝒅𝒕൪
Mem-Devices
• Charge-Controlled Memristor:ϕM(t) = fM(qM)
iM = dqM/dt, vM = dϕM/dt
• Flux-Controlled Memristor:qM(t) = fM(ϕM)
iM = dqM/dt, vM = dϕM/dt
Mem Systems
– Current-Controlled Memristive System: vM = f1(x,iM,t)iM(t)
dx/dt= f2(x,iM,t)
– Voltage-Controlled Memristive System: iM = f1(x,vM,t)vM(t)
dx/dt= f2(x,vM,t)
Memcapacitive Systems
• Voltage-Controlled Memcapacitive System:qM = f1(x,vM,t)vM(t)
iM = dqM/dt dx/dt= f2(x,vM,t)
• Charge-Controlled Memcapacitive System:vM = f1(x,qM,t)qM(t)
iM = dqM/dt dx/dt= f2(x,qM,t)
Meminductive Systems
• Current-Controlled Meminductive System:ϕM = f1(x,iM,t)iM(t)
vM = dϕM/dt dx/dt= f2(x,iM,t)
• Flux-Controlled Meminductive System:vM = f1(x,ϕM,t)ϕM(t)
iM = dqM/dt dx/dt= f2(x,ϕM,t)