- 2080 Bhadra · 4 marks
F-V and F-I analogy of mass-spring-damper system
Short answer
F-V analogy: force → voltage, mass → inductor, damper → resistor, spring → capacitor; mesh circuit has L=M with C1=1/K1, R2=B2, C2=1/K2. F-I analogy: force → current, mass → capacitor, damper → conductance (1/R), spring → inductor; node circuit has C=M, L1=1/K1, R2=1/B2, L2=1/K2.
Develop F-V and F-I analogy circuit of the mechanical system shown below. [Figure: force f applied to mass M (displacement X1, on rollers on ground); M connected through spring K1 to a point of displacement X2; from that point, damper B2 in parallel with spring K2 connect to the fixed wall]
Take (mass) and (junction of , , ) as the two displacements. The junction has no mass.
Equations of motion
F-V analogy (mesh/loop)
, , , , . Each displacement gives one mesh; is common to both.
with , , , .
L = M R2 = B2
+---LLLL----+---------/\/\/----+
| | |
(~) e C1=1/K1 C2=1/K2
| i1 | i2 |
+-----------+------------------+
F-I analogy (node)
, , , , . Each displacement gives one node; joins the nodes.
with , , , .
v1 L1=1/K1 v2
+---+--------LLLL-------+--------+
| | | |
(i) C=M R2=1/B2 L2=1/K2
| | | |
+---+-------------------+--------+ ground
✓ Answer checked by Claude Opus 5.5 (high effort)
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