Small Loop Efficiency, Q & Bandwidth
A comprehensive guide to understanding the performance characteristics of small transmitting loop antennas, including efficiency, Q-factor, and bandwidth relationships.
What is a Small Transmitting Loop?
A small transmitting loop (STL) is a loop antenna where the circumference is significantly smaller than one wavelength (typically less than 0.1λ). These compact antennas are popular among amateur radio operators for:
- Portability - Easy to transport and deploy
- Small footprint - Ideal for apartments, HOAs, and limited spaces
- Low noise - Excellent rejection of local electrical noise
- Directional pattern - Useful null for QRM rejection
A loop is considered "small" when its circumference is less than 0.1λ (lambda). For example, at 14 MHz (20m band), a loop with a 1-meter diameter has a circumference of about 3.14m, which is approximately 0.047λ (4.7% of a wavelength).
Understanding Efficiency
Antenna efficiency (η) is the ratio of radiated power to input power. In a small loop, efficiency is determined by the relationship between radiation resistance and loss resistance.
The Efficiency Formula
η = Rr / (Rr + Rloss)
Where:
- η (eta) = Efficiency (as a decimal, 0 to 1)
- Rr = Radiation resistance (ohms)
- Rloss = Total loss resistance (ohms)
Radiation Resistance
For a small loop, radiation resistance is very small and depends on the loop area and frequency:
Rr ≈ 31,171 × (A/λ²)²
Where:
- A = Loop area (m²)
- λ = Wavelength (m)
- Rr = Radiation resistance (Ω)
Radiation resistance increases with the fourth power of frequency for a fixed loop size. This is why small loops work better on higher frequencies - a 1m loop at 28 MHz has 4× the radiation resistance of the same loop at 14 MHz!
Loss Resistance
Loss resistance comes primarily from two sources:
- Conductor losses - RF resistance of the loop conductor (skin effect)
- Capacitor ESR - Equivalent series resistance of the tuning capacitor
Total Loss Resistance
Rloss = Rconductor + Rcapacitor
Where both components increase with frequency due to skin effect and capacitor Q degradation.
Worked Example: 20m Loop
Let's calculate the efficiency of a typical 20-meter magnetic loop:
Parameters:
- Frequency: 14.2 MHz (20m band)
- Loop shape: Circular
- Loop diameter: 1.0 meter
- Conductor: Copper tubing, 12mm diameter
- Capacitor: Air variable, ESR = 0.05Ω
Step 1: Calculate wavelength
- λ = c/f = 299,792,458 m/s / 14,200,000 Hz = 21.1 m
Step 2: Calculate loop area
- A = π × (d/2)² = π × (0.5)² = 0.785 m²
Step 3: Calculate radiation resistance
- Rr = 31,171 × (0.785 / 21.1²)² = 31,171 × (0.001765)² = 0.097Ω
Step 4: Estimate conductor loss
- Skin depth at 14.2 MHz in copper ≈ 17.4 μm
- RF resistance per meter ≈ 0.034 Ω/m
- Loop circumference = πd = 3.14 m
- Rconductor = 0.034 × 3.14 = 0.107Ω
Step 5: Total loss resistance
- Rloss = 0.107 + 0.05 = 0.157Ω
Step 6: Calculate efficiency
- η = 0.097 / (0.097 + 0.157) = 0.097 / 0.254 = 38.2%
Small transmitting loops typically achieve 20-50% efficiency on HF bands. While this might seem low, the compact size and excellent noise rejection often make the trade-off worthwhile. A well-designed loop can still deliver excellent performance!
Understanding Q-Factor
The Q-factor (quality factor) of a small loop is extremely high, which has both advantages and disadvantages.
Q-Factor Formula
Q = XL / Rtotal = 2πfL / (Rr + R loss)
Where:
- XL = Inductive reactance of the loop (Ω)
- Rtotal = Total resistance (radiation + loss)
- f = Operating frequency (Hz)
- L = Loop inductance (H)
What Q-Factor Means
- High Q (200-400): Very narrow bandwidth, excellent selectivity, difficult to tune
- Medium Q (100-200): Balanced bandwidth and tuning ease
- Low Q (<100): Wider bandwidth, easier tuning, but typically larger loop
Our example loop at 20m typically has a Q around 300, which is considered very high.
Bandwidth Relationships
Bandwidth and Q-factor are inversely related:
BW = f0 / Q
For our 20m loop example:
- Q = 300
- f0 = 14.2 MHz
- BW = 14,200,000 / 300 = 47.3 kHz (2:1 SWR bandwidth)
With a 47 kHz bandwidth, this loop covers most of the 20m band (14.0-14.35 MHz = 350 kHz) but requires retuning when changing frequency by more than ~25 kHz. This is typical for small loops and why a quality variable capacitor is essential!
Trade-offs and Design Considerations
Size vs. Efficiency
| Loop Diameter | Efficiency @ 20m | Q-Factor | Bandwidth | | ------------- | ---------------- | -------- | --------- | | 0.5m | ~15% | ~400 | ~35 kHz | | 1.0m | ~38% | ~300 | ~47 kHz | | 1.5m | ~58% | ~220 | ~65 kHz |
Doubling the loop diameter approximately quadruples the radiation resistance and more than doubles the efficiency. However, portability decreases significantly.
Conductor Diameter vs. Loss
Larger conductor diameter reduces RF resistance:
| Conductor Size | Rconductor @ 20m | Effect on Efficiency | | -------------- | --------------------------- | -------------------- | | 6mm copper | 0.21 Ω/m | ~30% efficient | | 12mm copper | 0.11 Ω/m | ~38% efficient | | 25mm copper | 0.05 Ω/m | ~45% efficient |
Capacitor Quality
The capacitor ESR directly impacts efficiency:
| Capacitor Type | Typical ESR | Loss Impact | | --------------- | ----------- | ------------------- | | Air variable | 0.02-0.05Ω | Minimal (~2% loss) | | Vacuum variable | 0.01-0.02Ω | Negligible | | Butterfly | 0.05-0.10Ω | Moderate (~5% loss) |
Small loops concentrate high RF voltage across the tuning capacitor. At 100W transmit power with Q=300, the capacitor can see 1,500V RMS or more! Always use a capacitor rated for at least 3-5kV for QRP operation, and 10kV+ for 100W+.
Practical Design Guidelines
For Maximum Efficiency
- Make the loop as large as practically possible
- Use the largest diameter conductor you can manage
- Choose a high-quality capacitor (vacuum or air variable)
- Minimize all connections and joints
- Consider higher frequencies (better efficiency at 20m than 40m)
For Maximum Bandwidth
- Reduce the Q by using thicker conductors
- Accept slightly lower efficiency
- Consider a larger loop diameter
- Use lossier (but voltage-safe) coupling methods
For Portability
- Accept lower efficiency (20-30% is still usable)
- Target QRP power levels (5-25W)
- Use collapsible or sectional construction
- Balance weight vs. conductor size
Verification and Testing
After building a loop, verify performance with:
- SWR meter - Check resonance and bandwidth
- Dummy load + multimeter - Measure capacitor voltage (check Q calculation)
- On-air testing - Compare signal reports to other antennas
- Professional antenna analyzer - Measure impedance, Q, and efficiency
Want to see how these formulas work in practice? Use our
Magnetic Loop Calculator
to experiment with different designs and see real-time efficiency, Q, and bandwidth calculations!
Further Reading
Academic References
- AA5TB Magnetic Loop Calculator - Steve Yates, AA5TB (comprehensive formula derivations)
- ARRL Antenna Book - Chapter on Small Transmitting Loops
- "Small Transmitting Loop Antennas" by Dr. Brian Austin, VP9MA
Online Resources
- AA5TB Loop Antenna Calculator - Reference standard for loop calculations
- Small Loop Resources - Frank Dörenberg's comprehensive guide
- QRP Labs Loop Projects - Practical construction examples
Related HamCalc Articles
- Dipole Antenna Tuning Guide - Compare loop vs. dipole characteristics
- Materials Library - Conductor and capacitor specifications
- RF Safety Guidelines - Safe operating distances
Summary
Small transmitting loops offer excellent performance in compact packages, with these key characteristics:
- Efficiency: 20-50% typical on HF, determined by Rr vs. Rloss
- Q-Factor: Very high (200-400), leading to excellent selectivity
- Bandwidth: Narrow (30-70 kHz at 20m), requiring retuning across bands
- Trade-offs: Size vs. efficiency vs. portability
Understanding these relationships allows you to design a loop that meets your specific needs, whether that's maximum efficiency, maximum portability, or a balanced compromise.
Ready to design your own loop? Try the Magnetic Loop Calculator to experiment with parameters and optimize your design!