nanovna

NanoVNA practical guide for real measurements

If you bought a NanoVNA to “check SWR,” you’re already on the right track—but a NanoVNA can do much more than show a single SWR number. Used correctly, it’s a compact vector network analyzer (VNA) that measures complex impedance versus frequency, plots S11 (reflection) and S21 (transmission), and lets you diagnose antenna/feedline problems, build better chokes, validate filters, and verify coax loss—without guessing.

This guide is written to be practical. It focuses on what matters in real installations: calibration discipline, reference plane control, connector quality, sweep settings, and repeatable methods for antennas, coax, and ferrites.

NanoVNA basics and real-world expectations

A NanoVNA generates a swept RF signal and measures amplitude and phase at its ports. From that, it derives scattering parameters:

  • S11: how much signal reflects back from the load (antenna, device under test). This is what you use for impedance, return loss, SWR, resonance.

  • S21: how much signal passes through the device (filter, cable, attenuator). This is insertion loss/gain and phase response.

What it’s excellent for

  • Antenna tuning (resonant frequency, bandwidth trends, matching network verification)

  • Feedline diagnostics (coax loss trends, velocity factor estimates, bad connectors)

  • Building and validating common-mode chokes (ferrite impedance vs frequency)

  • Measuring filters (bandpass, lowpass, notch), attenuators, couplers (S21 shape)

  • Comparing “before vs after” modifications in a repeatable way

What it’s not great for

  • Ultra-low-loss measurements at the edge of its dynamic range (e.g., tiny ripple in a high-performance cavity filter)

  • Precision metrology across wide frequency ranges without disciplined fixtures

  • Any measurement with sloppy connectors/adapters (it will faithfully measure your adapter chain’s mistakes)

A mindset that prevents 80% of frustration

A NanoVNA is only as “truthful” as your calibration reference plane and your RF mechanics (connectors, adapters, strain relief). Treat calibration like a habit, not a menu option you click once.

Hardware hygiene: connectors, adapters, cables

Most NanoVNA accuracy complaints are actually connector and adapter problems. At VHF/UHF, a single poor SMA adapter can introduce measurable errors; at HF, the electrical behavior still matters, especially when you’re chasing small changes.

Use fewer adapters than you think

Every extra mechanical interface adds:

  • additional mismatch

  • extra electrical length

  • more opportunity for looseness, oxidation, or off-spec geometry

Practical rule: keep the adapter chain as short and as consistent as possible. If you must use adapters, use high-quality pieces and keep one “standard measurement chain” you always repeat.

Protect the NanoVNA’s SMA ports

The NanoVNA’s SMA connectors are not meant to be a mechanical load-bearing structure. Use:

  • a short, flexible pigtail as a sacrificial lead

  • strain relief so you don’t torque the port

  • “sacrificial” adapters you don’t mind replacing

Clean and tighten properly

  • Finger-tight is often not enough for stable measurements at higher frequencies.

  • Don’t over-torque without a proper tool, but ensure repeatable tightness.

  • If results change when you touch the connector, you have a mechanical problem, not a software problem.

Understanding the reference plane

The most important concept in practical VNA work is the reference plane (also called the calibration plane). When you calibrate, you are telling the VNA: “Assume everything up to this exact point is perfect or known.”

If you calibrate at the NanoVNA port, then add a long adapter chain afterward, your measurement includes that chain. If you calibrate with the chain attached, you “move” the reference plane to the far end of the chain.

Why it matters for antennas

If you are trying to tune an antenna, you want the reference plane to be at the antenna feedpoint (or as close as you can reasonably achieve). If your reference plane is at the shack end of a long coax, you are not measuring the antenna alone—you are measuring antenna + feedline transformations + feedline loss + common-mode behavior.

The practical approach

  • For quick “is it in the ballpark?” checks: calibrate at the device end you can reach.

  • For tuning and diagnosing: bring the NanoVNA to the antenna feedpoint or calibrate with a known fixture that models the feedline.

Calibration without pain: SOLT done right

Most NanoVNA units use a variant of SOLT calibration:

  • Short

  • Open

  • Load (50 Ω)

  • Thru (for two-port calibration)

You’ll commonly do:

  • one-port calibration (S11 only) for antennas and impedance work

  • two-port calibration (S11 + S21) for filters/cables and insertion loss work

Step-by-step one-port calibration (S11)

  1. Set the frequency range (start/stop) to the band or span you actually care about.

  2. Choose a reasonable number of points (more on this later).

  3. Enter calibration menu and select one-port calibration.

  4. Attach Open standard at the reference plane, measure Open.

  5. Attach Short standard, measure Short.

  6. Attach 50 Ω Load standard, measure Load.

  7. Save/activate the calibration.

Key discipline: if you change the frequency span significantly, recalibrate. Calibrations are not magic universal offsets.

Step-by-step two-port calibration (S21)

Two-port work is where NanoVNA becomes shockingly useful, but also where sloppiness shows up fast.

  1. Set frequency span for your device (e.g., 1–60 MHz for HF filters; 100–500 MHz for VHF filters).

  2. Select two-port calibration (Open/Short/Load on each port, plus Thru).

  3. Perform Open/Short/Load on port 1 at the reference plane.

  4. Perform Open/Short/Load on port 2 at the reference plane.

  5. Connect a good Thru between port 1 and port 2 at the reference plane and measure Thru.

  6. Save/activate.

Practical tip: “Thru” should be as short and clean as possible. A random long patch cable is not a proper thru unless you calibrate with it intentionally and keep it fixed.

What to do when you don’t trust your calibration kit

Many NanoVNA kits ship with standards that are “good enough” for hobby use, but can vary. You can still do reliable comparative work if you:

  • keep the same standards for all tests

  • keep the same reference plane

  • focus on repeatability and trends

If you want higher confidence, upgrade to better SMA standards and keep them protected.

Sweep settings that actually matter

Frequency span and resolution

A too-wide span wastes resolution where you need it. A too-narrow span can hide multi-band behavior.

Practical workflow:

  • Use a wide scan to find resonances and general behavior.

  • Zoom into the region that matters and recalibrate for best accuracy.

Number of points

More points generally means better curve detail but slower sweeps and sometimes more noise depending on the device.

A good starting point:

  • 201–401 points for quick checks

  • 801–1024 points for detailed tuning or filter shape analysis

IF bandwidth and trace stability

Many VNAs allow IF bandwidth control (or an equivalent smoothing setting). Narrower IF bandwidth:

  • reduces noise

  • slows sweep

  • improves trace readability for low-level measurements

Use narrower IF bandwidth when you see jittery traces and you care about small variations.

Averaging and smoothing

Smoothing is not a substitute for proper calibration. Use it only to make the display readable, not to “fix” bad mechanics.

Reading the data: SWR, return loss, impedance, Smith chart

SWR is convenient but incomplete

SWR is derived from reflection coefficient magnitude. It does not tell you:

  • whether you’re resistive or reactive

  • what the actual impedance is

  • whether a change is due to the antenna or feedline transformations

SWR is a “symptom,” not a diagnosis.

Return loss gives you a more honest feel

Return loss (dB) is a logarithmic measure of reflected power. It’s often more useful for comparing changes:

  • 10 dB return loss is okay for many practical setups

  • 15–20 dB is good

  • 25–30 dB is excellent (but don’t obsess if it costs bandwidth or increases loss elsewhere)

Complex impedance is where the truth lives

The NanoVNA can show R + jX:

  • R (resistance) near 50 Ω at resonance is what you want for a 50 Ω system

  • X (reactance) crossing zero indicates resonance

Smith chart is not scary when you use it correctly

Think of the Smith chart as a map:

  • the center is 50 Ω resistive

  • left side is lower resistance

  • right side is higher resistance

  • above/below the center indicate inductive/capacitive reactance (depending on convention)

For antenna work:

  • watch how the impedance trace moves as you trim length or adjust matching

  • aim to bring the trace near the center at your target frequency

  • don’t expect a single perfect point across a wide bandwidth unless the antenna design supports it

Antenna measurements: doing it without fooling yourself

Measure at the feedpoint when possible

If you can bring the NanoVNA to the antenna feedpoint, you eliminate many confusing variables. Even a short temporary coax pigtail is easier to handle than “mystery transformations” from a long feedline.

If you must measure from the shack end

Be honest about what you are measuring:

  • the feedline transforms impedance as a function of electrical length

  • loss makes mismatches look “better” than they are

  • common-mode currents can shift resonance and distort readings

Shack-end measurements are still useful for:

  • verifying that a tuned system hasn’t drifted

  • detecting big changes (water ingress, broken connection, loose PL-259)

  • comparing configurations consistently

Common-mode currents: the invisible troublemaker

If you touch the feedline and the resonance shifts, or if the curve changes when the coax is routed differently, you likely have common-mode current on the outside of the shield.

Fixes (in order of effectiveness):

  • place a common-mode choke at the feedpoint

  • ensure proper balun/unun choice (and understand what it does)

  • improve counterpoise/radial system for end-fed or vertical antennas

  • avoid routing coax parallel to radiating elements when possible

A simple repeatable antenna tuning workflow

  1. Choose the band and set a narrow span around it (e.g., 6.8–7.3 MHz for 40 m).

  2. One-port calibrate at the closest practical reference plane.

  3. Observe R and X across the span.

  4. Adjust antenna length to move resonance (X=0 point) to target.

  5. Adjust matching to bring R closer to desired system impedance.

  6. Re-measure after each change; keep a small log of what you changed.

This avoids “random walking” and makes tuning predictable.

Practical examples: what common antenna types look like on a NanoVNA

Half-wave dipole

You’ll typically see:

  • a clear resonance where reactance crosses zero

  • resistance near 50–75 Ω depending on height and environment

  • bandwidth and resonance shifting with height and nearby objects

End-fed half-wave (EFHW)

EFHW is sensitive to:

  • matching transformer design (unun ratio, losses, saturation)

  • counterpoise and common-mode behavior

  • feedline routing

On the NanoVNA, you may see:

  • resonance points that move unexpectedly

  • impedance swings that look “wild” without a proper choke/counterpoise

  • improvement after adding a real choke at the transformer output

Vertical with radials

Verticals can measure beautifully when the radial system is adequate. When it’s not, the NanoVNA often reveals:

  • lower radiation resistance than expected

  • unstable resonance when the environment changes (wet ground, nearby metal)

  • big differences between “radials deployed” and “radials missing” tests

Compact antennas in compromise environments

Attic antennas, short whips, and loaded designs often show:

  • narrow bandwidth (high Q)

  • strong reactance slope near resonance

  • sensitivity to small geometry changes

The NanoVNA helps you see whether you’re improving matching at the cost of loss, or actually improving the radiator’s efficiency.

Coax measurements: loss, velocity factor, and “is my cable okay?”

Measuring insertion loss (S21) of a coax

This is a solid, practical two-port measurement:

  • Port 1 → coax → Port 2

  • Two-port calibration at the ends of your test leads

  • Measure S21 across frequency

You’ll see insertion loss rising with frequency. Use this to:

  • compare cable types

  • detect damaged cable (unusually high loss or ripple)

  • validate connectors and terminations

Important: for meaningful coax loss numbers, maintain good impedance matching at both ends (or at least understand the limitations if you can’t).

Estimating velocity factor and electrical length

You can estimate VF by measuring phase delay or by looking at impedance transformations in a known setup. In practice:

  • it’s easiest to compare a known line against a reference

  • you can detect “this is not the cable type I thought it was”

  • you can approximate length when you have no other option

Don’t expect lab-grade time-domain accuracy; use it as a diagnostic and sanity check.

Detecting bad connectors and water ingress

Symptoms you may see:

  • unexpected ripple in S21 (standing waves from mismatches)

  • unstable readings when moving the cable

  • significant changes after re-terminating connectors

For outdoor coax issues, compare dry-day vs wet-day results. Water ingress often shows up as changed loss and altered impedance behavior.

Measuring filters and RF components with S21

A NanoVNA becomes a powerful RF bench tool when you measure:

  • low-pass filters (harmonic suppression)

  • band-pass filters (front-end selectivity)

  • notch filters (broadcast band rejection)

  • attenuators (flat loss across span)

  • duplexers (within dynamic range limits)

How to set up clean S21 measurements

  • Use two-port calibration with a short, clean Thru

  • Keep cables short and stable

  • Avoid extra adapters

  • Choose a span that covers the passband and the stopbands of interest

Interpreting common filter shapes

  • A good low-pass filter shows low insertion loss in the passband, then steep attenuation beyond cutoff.

  • A band-pass filter shows a “hump” around center frequency and attenuation outside it.

  • A notch shows a deep dip at the rejection frequency.

If you see unexpected ripple, suspect:

  • connector mismatch

  • poor shielding

  • too-long test cables

  • calibration plane mismatch

Ferrite choke measurement: the method that makes NanoVNA pay for itself

Common-mode chokes are often built by “rule of thumb,” but the NanoVNA lets you measure whether your choke actually has high impedance where you need it.

What you want from a common-mode choke

A choke’s job is to present a high impedance to common-mode current on the outside of coax. A practical target:

  • hundreds of ohms minimum

  • ideally 1–5 kΩ or more in the trouble band(s)

  • stable behavior without overheating at power

The exact target depends on system and environment, but “more is usually better” within practical limits.

The key concept: measure common-mode impedance, not differential

If you wrap coax through ferrites and then measure S11 like it’s a normal load, you might not be measuring what you think. The goal is to characterize impedance that the choke presents to the unwanted common-mode path.

A simple choke measurement jig (practical and repeatable)

One proven method uses a series fixture:

  • Build a small test fixture where the choke under test is placed in series with the NanoVNA port, forming a measurable impedance.

  • Alternatively, use a known resistor reference and measure changes across frequency.

A very practical approach for hobby-level work is:

  • make a short coax “sample” with the choke (ferrite beads or toroids) on it

  • keep geometry fixed and compare builds consistently

  • measure S11 with a known termination strategy and interpret impedance trends

If you want more rigorous measurement, build a dedicated fixture with a known resistor and measure the impedance of the choke as a two-terminal element, then compute impedance from the reflection coefficient. The details depend on your exact NanoVNA model and available ports, but the critical requirements are always the same:

  • define a clear reference plane

  • keep lead lengths short

  • keep geometry consistent

  • avoid stray capacitance and inductance dominating the result

What the impedance curve tells you

A good choke will show:

  • rising impedance over the band where ferrite loss and inductance contribute usefully

  • a broad peak rather than a razor-thin spike (spikes can be resonance artifacts)

  • behavior that matches your target band, not just “somewhere”

If your curve shows a sharp peak and then collapses, you may be seeing fixture resonance rather than real choke performance. Improve the fixture and reduce stray lead length.

Ferrite mixes in practical terms

Different ferrite materials have different permeability and loss profiles. In broad terms:

  • some mixes excel at HF for suppression and common-mode choking

  • others work better higher up (VHF/UHF)

For HF chokes, you often aim for a mix that provides substantial impedance across your operating band with good power handling and without excessive heating. The NanoVNA is your reality check: if your choke shows weak impedance where your station is noisy or unstable, change the design.

Toroid vs bead vs coax turns

  • Multiple turns through a toroid increases inductance quickly but can increase capacitance too.

  • Beads can be stacked to build broadband impedance.

  • “Turns” count and spacing matter. Tight bunching may increase capacitance and create resonant peaks.

Measure, don’t guess: build two variants, measure both, keep the better curve.

Attic and indoor antennas: what NanoVNA reveals that SWR meters hide

Indoor installations create strong coupling to:

  • foil-backed insulation

  • wiring in walls

  • metal roofing elements

  • gutters and downspouts

  • HVAC ducts

NanoVNA helps you see:

  • resonance shifting when you move the antenna by tens of centimeters

  • impedance changing dramatically across seasons (humidity, rain on roof materials)

  • how much your feedline is becoming part of the antenna

Stabilizing an indoor setup

  • Use a good feedpoint choke to prevent the feedline from radiating

  • Keep consistent routing for coax

  • Avoid running the antenna parallel and close to large metal structures

  • Accept that perfect “textbook” impedance may be unrealistic; focus on stable resonance and manageable mismatch with minimal extra loss

Interpreting “weird” traces: the most common causes

Symptom: resonance shifts when you touch the coax

Cause: common-mode current and feedline coupling
Fix: add or improve choke, refine counterpoise, improve feedpoint balance

Symptom: the curve looks jagged or noisy

Cause: poor connection, unstable adapter, too-wide IF bandwidth, low-quality load
Fix: tighten/replace connectors, narrow IF bandwidth, use better standards

Symptom: calibration seems to “expire”

Cause: you changed span, changed adapters, moved reference plane, or temperature/mechanics changed
Fix: recalibrate with the measurement chain exactly as used

Symptom: SWR looks good but performance is bad

Cause: feedline loss hiding mismatch, lossy matching, poor radiation efficiency
Fix: look at impedance, bandwidth behavior, and compare field results; measure loss if possible; reconsider antenna design

Symptom: multiple dips and peaks across the band

Cause: multi-resonance structures, coupling to surroundings, feedline radiation, trap interactions
Fix: isolate variables; measure at feedpoint; add choke; change placement; use narrower sweeps to study each feature

A measurement workflow that saves time

Build a “standard kit”

  • one or two known-good SMA cables

  • one known-good 50 Ω load (better than the cheapest kit load)

  • a short high-quality Thru

  • a couple of quality adapters you always use

  • optional: an SMA torque tool and a sacrificial pigtail

Keep a measurement log

Write down:

  • calibration span

  • points/IF bandwidth

  • reference plane setup

  • antenna configuration (height, placement, counterpoise, choke used)

This makes your results comparable across days and seasons.

Use comparative testing as your superpower

Even if absolute accuracy isn’t lab-grade, the NanoVNA excels at comparative evaluation:

  • choke A vs choke B

  • matching network rev 1 vs rev 2

  • feedline connector old vs new

  • antenna placement option 1 vs option 2

If you can repeat the setup, you can trust the trend.

Quick checklist: “my NanoVNA results don’t make sense”

  1. Did you calibrate at the correct span and keep the same measurement chain afterward?

  2. Are you using too many adapters?

  3. Are connectors tight and mechanically stable?

  4. Are you unintentionally measuring feedline effects (common-mode, transformations)?

  5. Did you move or touch the setup between measurements?

  6. Are you relying on SWR instead of impedance/return loss?

  7. Is your environment (attic metal, wiring) dominating the antenna?

Advanced tips for getting more trustworthy data

Use port extension when appropriate

Some VNAs offer port extension to compensate for a known cable delay. This can help if you must include a fixed cable but want the display to behave as if the reference plane is moved.

Use it carefully:

  • it’s not a substitute for proper calibration

  • it assumes the cable is stable and well-behaved

Recognize dynamic range limits in S21

Deep stopband measurements may be limited by the NanoVNA’s noise floor and leakage. If your filter claims 80 dB rejection, your NanoVNA may not prove it. You can still verify:

  • cutoff frequency

  • basic passband shape

  • relative improvement

  • presence of unwanted resonances

Don’t ignore the phase

Phase information can help you spot:

  • unexpected resonances

  • fixture artifacts

  • cable issues

You don’t need to be a mathematician—just notice when phase behavior looks inconsistent with a simple component.


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