Microwave amplifiers become much more interesting when you stop looking at them as a single gain number.
A broadband amplifier may provide excellent gain at one frequency and behave differently at another. As the input level increases, gain compression becomes important, the DC power consumption becomes significant, and thermal conditions can affect repeatability.
The Mini-Circuits ZVE-3W-183+ is a good device for demonstrating these effects because it covers 5.9 to 18 GHz and provides approximately 35 dB typical gain. Mini-Circuits specifies +34 dBm typical output power at 1 dB compression and +35 dBm typical saturated output power at 3 dB compression. The amplifier is a Class-A, four-stage design with internal voltage regulation.
This project turns the amplifier into the center of a small microwave characterization bench.
What We Want to MeasureThe basic experiment measures:
- Frequency response
- Small-signal gain
- Input and output VSWR
- Output power versus input power
- Approximate 1 dB compression point
- DC voltage and current
- Heatsink temperature
- Gain variation across the 5.9–18 GHz range
The manufacturer's typical data shows that gain is not perfectly constant across the band. For example, the published typical data gives approximately 36.1 dB at 5.9 GHz, 34.6 dB at 7 GHz, 33.4 dB around 9–12 GHz, and approximately 33.8 dB at 18 GHz.
That makes this device useful for demonstrating a real engineering concept: broadband does not mean perfectly flat.
RF Test SetupThe simplest setup is:
Signal Generator → Attenuator → ZVE-3W-183+ → Attenuator → Power Sensor / Spectrum Analyzer
For gain measurements, a VNA can be inserted into the measurement workflow.
A suitable VNA should support the frequency range being tested. If the instrument only reaches a lower frequency, simply limit the experiment to the overlapping range rather than extrapolating the amplifier's performance.
The attenuator at the amplifier input is particularly important. The manufacturer's maximum input RF power rating is +20 dBm. The amplifier has approximately 35 dB gain, so an input signal near the maximum rating could theoretically produce an output far beyond the intended operating region.
For this reason, start with a much lower input level and increase the signal gradually while monitoring the output.
Measuring Small-Signal GainStart at a low input power where the amplifier is clearly operating in its linear region.
For example:
- Frequency: 6 GHz
- Input power: approximately −20 dBm
- Measure output power
- Calculate::
Gain = POUT − PIN
If the measured output is approximately +14 dBm, the measured gain is approximately:
14 dBm − (−20 dBm) = 34 dB
Repeat the measurement at several frequencies.
A useful sweep is:
6 GHz7 GHz8 GHz9 GHz10 GHz12 GHz14 GHz16 GHz18 GHz
The resulting graph provides a much more useful picture than a single gain measurement.
Measuring CompressionNext, select one frequency, such as 10 GHz.
Increase the RF input power in small steps while recording output power.
At low input levels, output power should increase approximately 1 dB for every 1 dB increase in input power.
As the amplifier approaches compression, the output increase becomes smaller.
The 1 dB compression point is reached when the measured output power is approximately 1 dB below the extrapolated linear response.
Mini-Circuits specifies a typical output power at 1 dB compression of +34 dBm across the specified frequency range, although actual bench measurements can differ from typical specifications.
Adding an ESP32The ESP32 is not used to generate the 18 GHz RF signal.
Instead, it acts as the monitoring controller.
It can record:
- Supply voltage
- Supply current
- DC input power
- Heatsink temperature
- Test timestamp
This separation is important. The microwave path remains a 50 Ω RF system, while the ESP32 handles low-frequency instrumentation.
The DC input power can be calculated as:
PDC = VDC × IDC
For example, at 15 V and 2.2 A:
PDC ≈ 33 W
This is substantially higher than the RF output power, which is why thermal management matters for a Class-A amplifier.
The manufacturer's specification lists a typical supply current of 2.2 A and specifies that the supply should be capable of delivering 3 A during startup.
Thermal MonitoringAttach a temperature sensor to the heatsink rather than directly to an RF connector or the microwave enclosure.
The temperature should be logged together with RF measurements.
This makes it possible to answer a practical question:
Does the measured gain or output power change as the amplifier heats up?
The experiment should not be used to intentionally exceed the manufacturer's temperature limits. The specified maximum base-plate temperature is 85°C.
Why This Is UsefulThis project is useful for RF engineers, students, and microwave enthusiasts because it demonstrates the complete measurement chain rather than just the amplifier.
It also shows an important engineering principle:
A high-frequency RF system is not only about the RF device.
Cables, attenuators, connectors, calibration, impedance matching, power measurement, thermal conditions, and DC power delivery can all affect the final result.
The same measurement approach can later be adapted to other RF amplifiers.
Expected ResultsThe expected results should be compared against the manufacturer's published typical data rather than treated as guaranteed limits.
The datasheet specifies:
- Frequency range: 5.9–18 GHz
- Typical gain: 35 dB
- Gain flatness: ±1.4 dB typical
- Input VSWR: 1.5:1 typical
- Output VSWR: 1.2:1 typical
- Output power at 1 dB compression: +34 dBm typical
- Saturated output power: +35 dBm typical
- Noise figure: 5.5 dB typical
- OIP3: +44 dBm typical
- Supply voltage: 13–18 V
- Typical supply current: 2.2 A
These are useful reference values, but the actual result depends on frequency, temperature, instrumentation, calibration, cables, connectors, and test conditions.
Important RF Safety Note3 W of RF power at microwave frequencies is not a casual signal level.
Do not operate the amplifier with an unknown load or an improperly connected RF path. Use appropriate 50 Ω components, rated attenuators, terminations, cables, and measurement equipment.
Always follow the amplifier manufacturer's operating limits and the safety requirements of the laboratory.
The purpose of this project is controlled RF measurement, not free-space radiation.




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