AnythingOnline
📡
Free RF Lumped-Element Phase Shifter Tool RF & Microwave
100% Free • No Sign-Up

Free RF Lumped-Element Phase Shifter Tool

Calculate exact $L$ and $C$ component values for low-pass (phase delay) and high-pass (phase advance) symmetric T and $\pi$ phase shifting networks matching $50\Omega$ systems.

📡 Frequency & Phase Angle

MHz
Ω
°
Network Architecture

📊 Synthesized L & C Values

Series Elements
--
Two identical branches
Shunt Element
--
Center to ground
Target Phase Shift: -- °
Time Delay (τ = Δφ / 360f): -- ps
Center Frequency Return Loss: > 35 dB (VSWR < 1.04)
Transmission Line Wavelength: -- mm
Equivalent Line Length (Free Space): -- mm
Synthesizing phase shifter elements...
Design Synthesis Formulas:
Low-Pass T: L_series = [ Z_0 · tan(φ/2) ] / ω  |  C_shunt = sin(φ) / [ ω · Z_0 ]
Low-Pass Π: C_shunt = [ tan(φ/2) ] / [ ω · Z_0 ]  |  L_series = [ Z_0 · sin(φ) ] / ω
High-pass networks replace inductors with capacitors and vice-versa, producing true complementary phase shifts with zero group delay distortion.

Recommended Tools & Equipment

Tested hardware and components for high reliability

100% Free Tool Zero Sign-Up

1. Switched-Line & Lumped-Element Phase Shifter Architecture

In phased-array radar, beamforming antennas, and vector modulators, electronically steerable phase shifters adjust the relative RF phase across multiple antenna elements. While distributed microstrip delay lines are practical at microwave frequencies ($> 5 ext{ GHz}$), at VHF and UHF ($50 ext{ MHz} - 1 ext{ GHz}$), distributed transmission lines are prohibitively bulky.

Lumped-element $T$ and $Pi$ networks simulate transmission line phase delay and phase advance using discrete inductors ($L$) and capacitors ($C$). By switching between a Low-Pass (delay) and High-Pass (advance) filter with RF PIN diodes or RF GaAs/pHEMT switches, a digital phase bit delivers constant phase difference with matched $50Omega$ input/output impedance.

2. Symmetric T vs $Pi$ Network Synthesis

For a symmetric network with characteristic impedance $Z_0$ and phase shift $phi$ at angular frequency $omega = 2pi f_0$:

  • Low-Pass T-Network: $$L_{series} = rac{Z_0 cdot an(phi / 2)}{omega} quad ( ext{two series inductors})$$ $$C_{shunt} = rac{sin(phi)}{omega cdot Z_0} quad ( ext{one center shunt capacitor})$$
  • Low-Pass $Pi$-Network: $$C_{shunt} = rac{ an(phi / 2)}{omega cdot Z_0} quad ( ext{two shunt capacitors to ground})$$ $$L_{series} = rac{Z_0 cdot sin(phi)}{omega} quad ( ext{one series inductor})$$

3. High-Pass (Phase Advance) Complement

High-pass networks provide positive phase advance ($+phi$). Applying the high-pass dual transformation swaps $L leftrightarrow C$: $$C_{series, HP} = rac{1}{omega cdot Z_0 cdot an(phi / 2)}, quad L_{shunt, HP} = rac{Z_0}{omega cdot sin(phi)}$$ Pairing a $+22.5^circ$ High-Pass with a $-22.5^circ$ Low-Pass creates a net $45.0^circ$ differential phase bit with flat broadband frequency response and zero insertion loss ripple.

Frequently Asked Questions

Why are lumped-element phase shifters limited to under 180 degrees per stage?

As the phase shift approaches 180 degrees, tan(phi/2) approaches infinity, requiring impractically huge component values with near-zero operating bandwidth. Phase shifts >= 90 degrees are typically broken into two cascaded stages (e.g. 180° = two 90° bits or four 45° bits).

What type of inductors should be used in UHF phase shifters?

Use high-Q wirewound ceramic chip inductors (such as Coilcraft 0402HP / 0603HP series with Q > 60). Multilayer ferrite inductors have high internal resistance and low Self-Resonant Frequency (SRF), resulting in unacceptable insertion loss.

How does parasitic capacitance affect the phase shift accuracy?

At frequencies above 500 MHz, PCB pad capacitance (approx 0.2 to 0.5 pF) and switch off-capacitance (Coff ≈ 0.15 pF) add in parallel with shunt capacitors. Board layout must subtract pad capacitance from synthesized C values.

Can this circuit handle high RF transmit power?

Lumped phase shifters can handle 10W to 100W if using high-Q porcelain multilayer capacitors (ATC 100A/100B series) and heavy-gauge air-core inductors. Low-power versions (< 1W) use standard surface mount chip parts.