---
title: "Two-mass system transfer function and F-V analogy"
subject: "Control Systems"
chapter: 2
key: "semester_3/control_systems:tf-two-mass-k1k2b1b2"
source: https://www.bctengineer.com/q/semester_3/control_systems/tf-two-mass-k1k2b1b2
site: BCT Engineering
---

# Two-mass system transfer function and F-V analogy

Control Systems · Chapter 2: Component Modeling

- Asked in: 2082 Baisakh, 8+2 marks
- Video: [Translational Mechanical Systems (Solved Example)](https://www.youtube.com/watch?v=Av86LcNuiMQ) — Neso Academy
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/control_systems/tf-two-mass-k1k2b1b2
- Whole chapter: https://www.bctengineer.com/md/semester_3/control_systems/chapter-2

## Question

Obtain transfer function for the system as below considering displacement of mass M2 as output. Also develop Force-Voltage analogous circuit. [Figure: wall – spring K1 – mass m1 (force F applied, displacement x1, friction fc1 with ground) – spring K2 in series with damper B1 – mass m2 (displacement x2, friction fc2 with ground) – damper B2 – wall]

## Short answer

X2(s)/F(s) = K2 B1 / [ (K2 + B1s)(m1 s^2 + fc1 s + K1)(m2 s + fc2 + B2) + K2 B1{(m1+m2)s^2 + (fc1+fc2+B2)s + K1} ]. In force-voltage analogy, force → voltage, mass → inductor, friction/damper → resistor, spring → capacitor.

## Answer

**Assumptions:** $f_{c1}$, $f_{c2}$ are viscous friction coefficients of $m_1$, $m_2$ with the ground; $x_3$ is the displacement of the massless junction between $K_2$ and $B_1$ ($K_2$ on the $m_1$ side); zero initial conditions.

#### Equations of motion (Laplace form)
Mass $m_1$:

$$
F(s) = (m_1s^2 + f_{c1}s + K_1)X_1 + K_2(X_1 - X_3)
$$

Junction: $\;K_2(X_3 - X_1) + B_1s(X_3 - X_2) = 0$

Mass $m_2$:

$$
0 = (m_2s^2 + f_{c2}s + B_2s)X_2 + B_1s(X_2 - X_3)
$$

#### Solving
$K_2$ and $B_1$ in series carry the same force, so they act as one coupling element

$$
Z_c(s) = \frac{K_2B_1s}{K_2 + B_1s}
$$

Let $Z_1 = m_1s^2 + f_{c1}s + K_1$ and $Z_2 = m_2s^2 + (f_{c2}+B_2)s$. Then

$$
\begin{bmatrix} Z_1 + Z_c & -Z_c \\ -Z_c & Z_2 + Z_c \end{bmatrix}
\begin{bmatrix} X_1 \\ X_2 \end{bmatrix} = \begin{bmatrix} F \\ 0 \end{bmatrix}
$$

$$
\frac{X_2}{F} = \frac{Z_c}{(Z_1+Z_c)(Z_2+Z_c) - Z_c^2} = \frac{Z_c}{Z_1Z_2 + Z_c(Z_1 + Z_2)}
$$

Substituting $Z_c$, multiplying by $(K_2 + B_1s)$ and cancelling the common factor $s$:

$$
\frac{X_2(s)}{F(s)} = \frac{K_2B_1}{(K_2 + B_1s)(m_1s^2 + f_{c1}s + K_1)(m_2s + f_{c2} + B_2) + K_2B_1\left[(m_1+m_2)s^2 + (f_{c1}+f_{c2}+B_2)s + K_1\right]}
$$

The denominator is a fourth-order polynomial; its leading term is $B_1m_1m_2s^4$ and its constant term is $K_1K_2(B_1 + B_2 + f_{c2})$.

#### Force–voltage (F-V) analogy
Force → voltage, mass → $L$, friction/damper → $R$, spring → $C = 1/K$, velocity → loop current. Mechanical series ($K_2$, $B_1$) → electrical parallel ($C_2 \parallel R_{B1}$), shared by both loops.

```text
  +--[L1]--[Rf1]--[C1]--+--[L2]--[Rf2]--[RB2]--+
  |                     |                      |
 (F)  i1 ->          +--+--+          <- i2    |
  |                  C2   RB1                  |
  |                  +--+--+                   |
  |                     |                      |
  +---------------------+----------------------+
 L1=m1, Rf1=fc1, C1=1/K1, C2=1/K2, RB1=B1
 L2=m2, Rf2=fc2, RB2=B2
```

Loop equations, with $i = \dot x$:

$$
\begin{aligned}
F &= L_1\frac{di_1}{dt} + R_{f1}i_1 + \frac{1}{C_1}\int i_1dt + v_p \\
0 &= L_2\frac{di_2}{dt} + (R_{f2} + R_{B2})i_2 - v_p
\end{aligned}
$$

where $v_p$ is the voltage across $C_2 \parallel R_{B1}$ carrying $(i_1 - i_2)$ in total; these match the mechanical equations.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. K2 in series with B1 act as
   A. Zc(s) = K2 B1 s/(K2 + B1 s)
   B. K2 + B1 s
   C. K2 B1
   D. B1 s/K2
   Answer: A. Series elements share force. (Key point: Coupling element)

2. The denominator polynomial is of order
   A. two
   B. four, with leading term B1 m1 m2 s^4
   C. three, with leading term m1 m2 s^3
   D. five
   Answer: B. Two masses give s^2 each; B1 contributes one more s after cancelling. (Key point: Denominator order)

3. Mechanical series K2, B1 becomes
   A. series C2 and R_B1
   B. a single inductor
   C. electrical parallel C2 || R_B1 shared by both loops
   D. a voltage source
   Answer: C. Series to parallel in F-V analogy. (Key point: F-V analogy)

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