---
title: "Critical frequency; MUF and skip distance (flat earth)"
subject: "Propagation and Antenna"
chapter: 4
key: "semester_6/propagation_and_antenna:critical-frequency-skip-muf-flat"
source: https://www.bctengineer.com/q/semester_6/propagation_and_antenna/critical-frequency-skip-muf-flat
site: BCT Engineering
---

# Critical frequency; MUF and skip distance (flat earth)

Propagation and Antenna · Chapter 4: Propagation and Radio Frequency Spectrum

- Asked in: 2081 Chaitra, 2+6 marks; 2080 Chaitra, 2+7 marks (asked 2 times)
- Video: [Sky Wave Propagation 2 | Critical Frequency I MUF I Skip Distance | Optimum Frequency IAntenna Hindi](https://www.youtube.com/watch?v=VqgcHBtYorM) — Dopamine
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_6/propagation_and_antenna/critical-frequency-skip-muf-flat
- Whole chapter: https://www.bctengineer.com/md/semester_6/propagation_and_antenna/chapter-4

## Question

Define the critical frequency (fcr). Derive an expression for the relation between skip distance and maximum usable frequency (fmuf) in SW propagation assuming that the Earth is flat.

## Short answer

Critical frequency fcr = 9√Nmax is the maximum vertical-incidence frequency reflected by a layer. For flat earth, with virtual height h, MUF = fcr √(1 + D²/4h²) and skip distance D = 2h √[(fMUF/fcr)² − 1].

## Answer

#### Critical frequency
The **critical frequency (fcr)** of an ionospheric layer is the highest frequency that is reflected back to earth when the wave is sent **vertically upward**. Higher frequencies at vertical incidence pass through the layer. It depends on the maximum electron density of the layer:
```text
fcr = 9 √Nmax    (fcr in Hz, Nmax in electrons/m³)
```
Typical values: E ≈ 3–4 MHz, F2 ≈ 5–12 MHz.

#### Relation between skip distance and MUF (flat earth)
**Skip distance (D)** is the shortest distance from the transmitter at which a sky wave of a given frequency returns to earth. The **maximum usable frequency (f_MUF)** is the highest frequency that returns to earth for a given distance (angle of incidence).

Assumptions: earth and ionosphere are flat; reflection takes place at virtual height *h*; the path is symmetric (both antennas on ground).

```text
          ionosphere (virtual height h)
  ~~~~~~~~~~~~~~~~~~ P ~~~~~~~~~~~~~~~~~~
                   / | \
                  /θi|  \
                 /   |h  \
                /    |    \
   flat earth  T-----M-----R
               <--- D ---->
  TM = MR = D/2,  θi = angle of incidence
```

Refractive index of an ionised layer (electron density N per m³, frequency f in Hz):
```text
n = √(1 − 81N / f²)
```
By Snell's law, a wave entering at angle θi turns back where the ray becomes horizontal (refraction angle 90°):
```text
sin θi = n = √(1 − 81Nmax / f²)
cos² θi = 81Nmax / f²
f = 9√Nmax / cos θi
```
For vertical incidence (θi = 0) this gives the critical frequency fc = 9√Nmax, so
```text
f_MUF = fc sec θi          (secant law)
```
From the flat-earth geometry (triangle TMP):
```text
tan θi = (D/2) / h
sec θi = √(1 + tan² θi) = √(1 + D² / 4h²)

f_MUF = fc √(1 + D² / 4h²) = fc √(4h² + D²) / (2h)
```
Solving for the skip distance:
```text
(f_MUF / fc)² = 1 + D² / 4h²
D = 2h √[(f_MUF / fc)² − 1]
```

**Result**
```text
f_MUF = fcr √(1 + D²/4h²)
D     = 2h √[(f_MUF/fcr)² − 1]
```
- For f ≤ fcr, D = 0 (no skip zone).
- As frequency rises above fcr, the skip distance grows.

**Example:** h = 300 km, fcr = 8 MHz, f = 16 MHz: D = 2 × 300 × √(4 − 1) = 1039 km.

## Check yourself

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

1. What is the critical frequency?
   A. The highest frequency reflected at vertical incidence, fcr = 9√Nmax
   B. The lowest frequency absorbed by D layer
   C. The highest frequency at any incidence
   D. The frequency at which skip distance is largest
   Answer: A. Above fcr, a vertically sent wave passes through the layer. (Key point: Definition of critical frequency)

2. At the point of reflection, what is the refraction angle, and what does Snell's law give?
   A. 90°; sin θi = n = √(1 − 81Nmax/f²), so f = 9√Nmax / cos θi
   B. 0°; sin θi = 1
   C. 45°; f = fc
   D. 90°; sin θi = 81N/f²
   Answer: A. The ray turns horizontal, giving cos²θi = 81Nmax/f², so f = fc sec θi. (Key point: Condition at reflection)

3. From the flat-earth geometry, what is sec θi?
   A. √(1 + D²/4h²)
   B. √(1 + D²/h²)
   C. D/2h
   D. √(1 − D²/4h²)
   Answer: A. tan θi = (D/2)/h, so sec θi = √(1 + tan²θi) = √(1 + D²/4h²). (Key point: Flat-earth geometry)

4. What is the skip distance in terms of MUF?
   A. D = 2h √[(fMUF/fcr)² − 1]
   B. D = h √[(fMUF/fcr)² + 1]
   C. D = 2h (fMUF/fcr)
   D. D = h/2 √[1 − (fMUF/fcr)²]
   Answer: A. Solving fMUF/fcr = √(1 + D²/4h²) gives D = 2h√[(fMUF/fcr)² − 1]. Example: h = 300 km, fcr = 8 MHz, f = 16 MHz gives 1039 km. (Key point: Final result)

## Related in Propagation and Antenna

- [MUF, critical frequency and skip (curved earth)](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Amuf-fcr-skip-curved-earth) — Propagation and Antenna, chapter 4
- [Critical frequency and skip distance (flat earth)](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Acritical-frequency-skip-distance-flat) — Propagation and Antenna, chapter 4, asked 2×
- [MUF and skip distance (flat earth)](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Amuf-skip-distance-flat) — Propagation and Antenna, chapter 4, asked 2×
- [Skip distance derivation (flat earth)](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Askip-distance-flat-earth) — Propagation and Antenna, chapter 4, asked 2×
- [Skip distance and MUF (curved earth)](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Askip-muf-curved-earth) — Propagation and Antenna, chapter 4
- [MUF and critical frequency relation](https://www.bctengineer.com/question.md?key=semester_6%2Fpropagation_and_antenna%3Amuf-critical-frequency-relation) — Propagation and Antenna, chapter 4
