---
title: "Bode plot: 20(S+5)/(S(S²+2S+10)(S²+21S+20))"
subject: "Electrical Circuit Theory"
chapter: 5
key: "semester_3/electrical_circuit_theory:bode-20s5-s-s2-2s-10"
source: https://www.bctengineer.com/q/semester_3/electrical_circuit_theory/bode-20s5-s-s2-2s-10
site: BCT Engineering
---

# Bode plot: 20(S+5)/(S(S²+2S+10)(S²+21S+20))

Electrical Circuit Theory · Chapter 5: Frequency Response of Network

- Asked in: 2068 Shrawan, 8 marks
- Video: [1. Bode Plot Solved Example: Steps, Procedure, Parameters, and Stability](https://www.youtube.com/watch?v=lTnqZVNReF8) — Engineering Funda
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/electrical_circuit_theory/bode-20s5-s-s2-2s-10
- Whole chapter: https://www.bctengineer.com/md/semester_3/electrical_circuit_theory/chapter-5

## Question

Sketch the asymptotic Bode plots for the transfer function given by G(S) = 20(S + 5) / [S(S² + 2S + 10)(S² + 21S + 20)].

## Short answer

Time-constant form: 0.5(1+s/5)/[s(1+s)(1+s/20)(1+0.2s+s²/10)], 20log0.5=−6 dB. Corners: 1 (pole, −20 dB/dec), 3.16 rad/s (quad pole, ζ=0.316, −40 dB/dec), 5 (zero, +20), 20 rad/s (pole). Initial −20 dB/dec through −6 dB at ω=1, phase −90° to −360°, ~4 dB resonant peak.

## Answer

A Bode plot has two curves against log ω: the gain 20 log|H(jω)| in dB and the phase ∠H(jω). The asymptotic (straight-line) magnitude plot is drawn by writing H(s) in time-constant form, finding the corner frequencies and changing the slope by ±20 dB/decade for each simple factor (±40 for each quadratic factor).

#### Step 1: Standard form

```text
G(s) = 20(s + 5) / [ s (s² + 2s + 10)(s² + 21s + 20) ]
     = 20(s + 5) / [ s (s + 1)(s + 20)(s² + 2s + 10) ]   since s² + 21s + 20 = (s + 1)(s + 20)
```

```text
H(s) = 0.5 × (1 + s/5)
         / [ s (1 + s/1) (1 + s/20) (1 + 0.2 s + s²/10) ]
```

Constant term K₀ = 0.5, so 20 log K₀ = −6.02 dB.

#### Step 2: Corner frequencies

| Corner ω (rad/s) | Factor | Slope change |
|---|---|---|
| 1 | pole 1/(1 + s/1) | −20 dB/dec |
| 3.162 | quadratic pole, ωn = 3.162, ζ = 0.316 | −40 dB/dec |
| 5 | zero (1 + s/5) | +20 dB/dec |
| 20 | pole 1/(1 + s/20) | −20 dB/dec |

The quadratic s² + 2s + 10 has ωn = √10 = 3.162 rad/s and ζ = 0.316.

#### Step 3: Magnitude plot

The net number of poles at the origin is 1, so the low-frequency asymptote has slope −20 dB/decade and passes through −6 dB at ω = 1 rad/s. The slope then changes at each corner as below.

| ω (rad/s) | Slope after corner | Asymptotic gain (dB) | Phase (°) |
|---|---|---|---|
| 0.1 | −20 | 14 | −96 |
| 1 | −40 | −6 | −139 |
| 3.162 | −80 | −26 | −229 |
| 5 | −60 | −41.9 | −284 |
| 20 | −80 | −78.1 | −320 |

Asymptotic magnitude plot (each * is the asymptote; 1 row = 10 dB):

```text
  20 |                                     
     |******                               
   0 |      ******                         
     |            ***                      
 −20 |               ***                   
     |                  **                 
 −40 |                    **               
     |                      *              
 −60 |                       **            
     |                         **          
 −80 |                           **        
     |                             **      
−100 |                               *     
     |                                **   
−120 |                                  *  
     |                                   **
−140 |                                     
     ++-----------+-----------+-----------+
      0.1         1           10          100  ω (rad/s)
```

At ωn = 3.162 the quadratic pole has ζ = 0.316, so the true curve rises about 4 dB above the asymptote there (resonant peak, −20 log 2ζ); the actual peak is near ωn.

#### Step 4: Phase plot

Low-frequency phase = 90° × (zeros at origin − poles at origin) = −90°. Each simple factor changes the phase by 90° (zero: +, pole: −), spread over the range 0.1ωc to 10ωc with 45° at ωc; each quadratic factor changes it by 180°, with ±90° at ωn. High-frequency phase = 90° × (m − n) = −360°. Exact phase values at the corners are in the table above; join them with a smooth curve starting at −90° and ending at −360°.

Accuracy check: at the first corner ω = 1 rad/s the exact gain is −8.2 dB, the asymptote gives −6 dB.

## Check yourself

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

1. How does s^2 + 21s + 20 factor?
   A. (s+1)(s+20)
   B. (s+4)(s+5)
   C. (s+2)(s+10)
   D. (s+3)(s+7)
   Answer: A. 1 x 20 = 20 and 1 + 20 = 21. (Key point: Factoring)

2. What is K0?
   A. 2
   B. 0.5 (-6.02 dB)
   C. 20
   D. 0.05
   Answer: B. K0 = 20 x 5 /(1 x 20 x 10) = 0.5. (Key point: Constant term)

3. What is the slope just after omega_n = 3.162 (before 5)?
   A. -60 dB/dec
   B. -40 dB/dec
   C. -80 dB/dec
   D. -100 dB/dec
   Answer: C. -20 at start, -40 after the pole at 1, and -80 after the quadratic pole. (Key point: Slope after omega_n)

4. What is the high-frequency phase?
   A. -270 deg
   B. -180 deg
   C. -450 deg
   D. -360 deg
   Answer: D. 90 x (1 - 5) = -360 deg. (Key point: High-frequency phase)

## Close variants set in other exams

- [Bode plot: 2s²(S+5)/((S²+22S+40)(S+10))](https://www.bctengineer.com/question.md?key=semester_3%2Felectrical_circuit_theory%3Abode-2s2-s5-s2-22s-40) — Electrical Circuit Theory, chapter 5, asked 2×

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