T-Junction Power Divider
Overview
The simplest RF power divider using only transmission line impedance transformations. Provides matched input port but no isolation between outputs. Ideal for applications where isolation is not required and high power handling is needed.
Topology
┌──[Z₂, λ/4]── Port 2
│
Input ──[Z₀, λ/4]───┤
(Port 1) │
└──[Z₃, λ/4]── Port 3
Basic structure:
Input λ/4 line at Z₀
Two output λ/4 branches at Z₂, Z₃
Physical T-junction connection point
For unequal split, additional matching:
┌──[Z₂, λ/4]──[Z₂ₘ, λ/4]── Port 2
│
Input ──[Z₀, λ/4]───┤
│
└──[Z₃, λ/4]──[Z₃ₘ, λ/4]── Port 3
Design Equations
Power Split Ratio
K = P₂/P₃ = (Port 2 power / Port 3 power)
Branch Impedances (First Stage)
Matching Sections (Unequal Split Only)
For K ≠ 1, add λ/4 matching transformers:
Equal Split (K = 1)
Z₂ = Z₃ = 2 × Z₀
No additional matching needed
For Z₀ = 50 Ω:
Z₂ = Z₃ = 100 Ω
Critical: Ports 2 and 3 are directly connected through the junction, so there’s no isolation between them.
Advantages
Simplest design: Only transmission lines, no resistors
Low insertion loss: Only conductor/dielectric losses
Small size: Compact layout (equal split)
Low cost: No isolation resistors to specify/purchase
Limitations
No isolation: S₂₃ ≈ 0 dB
Signals at Port 2 leak directly to Port 3
Impedance at one output affects the other
Impedance mismatch
Comparison with Wilkinson
Feature |
T-Junction |
Wilkinson |
|---|---|---|
Isolation |
None (~0 dB) |
Excellent (>20 dB) |
Components |
TL only |
TL + Resistor |
Power handling |
Very high |
Limited by R |
Insertion loss |
Very low |
Low |
Complexity |
Simplest |
Simple |
Bandwidth |
Narrow (10-15%) |
Medium (20-40%) |
Combining |
Cannot combine |
Can combine |
Cost |
Lowest |
Low |
References
[1] Pozar, D. M. (2012). Microwave Engineering (4th ed.), Section 7.3. Wiley.