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Lumped Modeling with Circuit Elements, Ch. 5, Text

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Lumped Modeling with Circuit Elements, Ch. 5, Text. Ideal elements represent real physical systems. Resistor, spring, capacitor, mass, dashpot, inductor… To model a dynamic system, we must figure out how to put the elements from different domains together. - PowerPoint PPT Presentation
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Lumped Modeling with Circuit Elements, Ch. 5, Text • Ideal elements represent real physical systems. – Resistor, spring, capacitor, mass, dashpot, inductor… – To model a dynamic system, we must figure out how to put the elements from different domains together. – Alternatives include numerical modeling of the whole system. Lumped element modeling offers more physical insight and may be necessary for timely solutions.
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Page 1: Lumped Modeling with Circuit Elements, Ch. 5, Text

Lumped Modeling with Circuit Elements, Ch. 5, Text

• Ideal elements represent real physical systems.– Resistor, spring, capacitor, mass, dashpot,

inductor…– To model a dynamic system, we must figure out

how to put the elements from different domains together.

– Alternatives include numerical modeling of the whole system. Lumped element modeling offers more physical insight and may be necessary for timely solutions.

Page 2: Lumped Modeling with Circuit Elements, Ch. 5, Text

Example. Electrical: Resistor-Inductor-Capacitor (RLC) system.

R L

CNo power source, transient response depends on initial conditions

B1, B2 depend on initial conditions

i

Page 3: Lumped Modeling with Circuit Elements, Ch. 5, Text

Example. Mechanical: Spring-Mass-Dashpot system.

k

m

b

B1, B2 depend on initial conditions

No power source, transient response depends on initial conditions

x

Page 4: Lumped Modeling with Circuit Elements, Ch. 5, Text

Equations are the same if:

k

m

b

b m

1/k

R L

C1/C

L

R

or

x.

I <-> x.

Page 5: Lumped Modeling with Circuit Elements, Ch. 5, Text

Goal: Simulate the entire system.

• Usual practice:– Write all elements as electrical circuit elements.– Represent the intradomain transducers (Ch. 6)– Use the powerful techniques developed for circuit

analysis, linear systems (if linear), and feedback control on the whole MEMS system.

Page 6: Lumped Modeling with Circuit Elements, Ch. 5, Text

Senturia generalizes these ideas.• Introduce conjugate power variables, effort,

e(t), and flow, f(t).• Then, generalized displacement, q(t)• And generalized momentum, p(t)

e . f has units of powere . q has units of energyp . f has units of energy

Page 7: Lumped Modeling with Circuit Elements, Ch. 5, Text
Page 8: Lumped Modeling with Circuit Elements, Ch. 5, Text

Variable Assignment Conventions• Senturia uses e -> V, that is, effort is linked

with voltage in the electrical equivalent circuit. He explains the reasons (for example potential energy is always associated with energy storage in capacitors).

Page 9: Lumped Modeling with Circuit Elements, Ch. 5, Text

Following Senturia’s e -> V convention:• For effort source, e is independent of f

• For flow source, f is independent of e

• For the generalized resistor, e=e(f) or f=f(e)

• Linear resistor e=Rf• Electrical, V=RI• Mechanical, F=bV

Page 10: Lumped Modeling with Circuit Elements, Ch. 5, Text

• For the generalized capacitor (potential energy):

•For a linear electrical capacitor:

ε – permitivityA – areaG – Gap

Page 11: Lumped Modeling with Circuit Elements, Ch. 5, Text

•The mechanical equivalent is the linear spring.

(Check in table.)

Cspring = 1/k

Page 12: Lumped Modeling with Circuit Elements, Ch. 5, Text
Page 13: Lumped Modeling with Circuit Elements, Ch. 5, Text

•Generalized Inductor or inertance (kinetic energy?)

Linear inertance: momentum

m – massv – velocityp – momentum

Electrical?

But what is this???

???

flow momentum?

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