class 5 - 6 analogous systems

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System Modeling Coursework

P.R. VENKATESWARANFaculty, Instrumentation and Control Engineering,

Manipal Institute of Technology, ManipalKarnataka 576 104 INDIAPh: 0820 2925154, 2925152

Fax: 0820 2571071Email: pr.venkat@manipal.edu, prv_i@yahoo.com

Blog: www.godsfavouritechild.wordpress.comWeb address: http://www.esnips.com/web/SystemModelingClassNotes

Class 5-6 : Analogous Systems

July – December 2008 prv/System Modeling Coursework/MIT-Manipal 2

WARNING!

I claim no originality in all these notes. These are the compilation from various sources for the purpose of delivering lectures. I humbly acknowledge the wonderful help provided by the original sources in this compilation.

For best results, it is always suggested you read the source material.

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Contents

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What is meant by analogous systems?

It is possible to make electrical and mechanical systems using analogs.

An analogous electrical and mechanical system will have differential equations of the same form.

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Analogous Quantities

Electrical

Quantity

Mechanical

Analog I

(Force-Current)

Mechanical

Analog II

(Force Voltage)

Voltage, e Velocity, v Force, f

Current, i Force, f Velocity, v

Resistance, R Lubricity, 1/B

(Inverse friction) Friction, B

Capacitance, C Mass, M Compliance, 1/K

(Inverse spring constant)

Inductance, L Compliance, 1/K

(Inverse spring constant) Mass, M

Transformer, N1:N2 Lever, L1:L2 Lever, L1:L2

July – December 2008 prv/System Modeling Coursework/MIT-Manipal 6

Analogous quantities in force(Torque)-Voltage Analogy

Mechanical Translational systems

Mechanical rotational Systems Electrical System

Force F Torque, T Voltage, e

Mass, M Moment of inertia J Inductance L

Viscous Friction Coefficient B

Viscous Friction Coefficient B Resistance R

Spring stiffness K Torsional

spring stiffness K Reciprocal of capacitance 1/C

Displacement x Angular Displacement, θ Charge q

Velocity, v Angular Velocity, ω Charge i

July – December 2008 prv/System Modeling Coursework/MIT-Manipal 7

Analogous quantities in Force (Torque)-Current Analogy

Mechanical Translational systems

Mechanical Rotational Systems

Electrical System

Force F Torque, T Current, i

Mass, M Moment of inertia J Capacitance C

Viscous Friction Coefficient B

Viscous Friction Coefficient B Reciprocal of Resistance 1/R

Spring stiffness K Torsional

spring stiffness K Reciprocal of inductance 1/L

Displacement x Angular Displacement, θ Magnetic flux linkage φ

Velocity, v Angular Velocity, ω Voltage e

July – December 2008 prv/System Modeling Coursework/MIT-Manipal 8

Converting between systems

The important relationship when converting from a circuit to the Mechanical 1 analog is that between Kirchoff's

Current Law and

D'Alemberts

Law (with inertial forces included).

Electrical Mechanical 1

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Procedure for Conversion from Electrical to Mechanical

The conversion from an electrical circuit to a mechanical analog is easily accomplished if capacitors in the circuit are grounded.

If they are

not, the process results in a mechanical system where positions must be chosen very carefully and the process can be much more difficult.

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Procedure for Conversion from Electrical to Mechanical

Start with an electrical circuit.

Label all node voltages

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Procedure for Conversion from Electrical to Mechanical

Write a node equations for each node voltage

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Procedure for Conversion from Electrical to Mechanical

Re-write the equations using analogs (make making substitutions from the table of analogous quantities), with each electrical node being replaced by a position.

July – December 2008 prv/System Modeling Coursework/MIT-Manipal 13

Procedure for Conversion from Electrical to Mechanical

Draw the mechanical system that corresponds with the equations.

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Mechanical (Force-Current) to Electrical Conversion

Start with the mechanical system. Label all

positions.

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Mechanical (Force-Current) to Electrical Conversion

Draw over circuit, replacing mechanical elements with their analogs; force generators by current sources, input velocities by voltage sources,

friction elements by resistors, springs by inductors, and masses by capacitors (which are grounded).

Each position becomes a node.

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Mechanical (Force-Current) to Electrical Conversion

Label nodes and electrical elements as they were in the original mechanical system.

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Verification of Mechanical to Electrical Analog

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Verification of Mechanical to Electrical Analog

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Numerical No.1 Convert into Mechanical equivalent

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Summary

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References

• http://www.swarthmore.edu/NatSci/echeeve1/A

nalogous Electrical and Mechanical Systems•

http://www.swarthmore.edu/NatSci/echeeve1/R

ef/Analogs/ElectricalMechanicalAnalogs.html#Q uantities#Quantities

amongst others…

July – December 2008 prv/System Modeling Coursework/MIT-Manipal 22

And, before we break…

The unexamined life is not worth living–

Socrates

Thanks for listening…

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