A field team faces an unresolved physical question: Why can a 22.5 dBm bench pass become 20.0 dBm in the enclosure? They must answer it before changing installed antenna gain on the real device. Predict the direction first.
See the relationship before changing it
The figure reads from left to right. The blue card is installed antenna gain. The middle card applies this page's relationship. The green card is installed eirp. Walk the arrows once: set the input, apply the rule, then read the result with its unit.
The retained audit below checks several chapter fixtures. This added model holds every other chapter fixture fixed, so the numeric fixture does not switch without explanation.
Derive the baseline in four named moves
- 1
Name the input. The chapter baseline for installed antenna gain is -3.
- 2
Name the relationship. Pport=Pt-Lcable; EIRP=Pt+Ginstalled; R=10^((Pport-EIRP)/10)
- 3
Substitute the chapter fixture. Set installed antenna gain to -3. The page ledger gives installed eirp as 20.00 dBm.
- 4
Read the result. Keep dBm beside the value. Use it only inside the technical boundary on this page.
Predict, then change installed antenna gain
Try Predict the direction of installed eirp. Move one control, calculate, then check your prediction.
Observe The slider cannot change the conducted test because the antenna is outside that measurement plane. It changes only the installed radiated budget. Reset the control to -3 and compare installed eirp.
Explain Only installed antenna gain moves here. The other chapter fixtures remain fixed.
Check yourself
What should you do before trusting a moved-control result?
What does this small model leave out?
1. Name the measurement plane
A cable into a test set ends before the antenna. An over-the-air budget includes the installed antenna. Both can be reported in dBm, but they describe different physical planes.
2. Name the algebra moves
Subtract cable lossPport=Pt−Lcable.
Add installed gainEIRP=Pt+Ginstalled.
Form the gapΔ=Pport−EIRP.
Undo decibelsR=10^(Δ/10).
3. Reproduce the bench and enclosure
The 2.50 dB difference is a 1.78× bench-to-radiated power ratio. It does not say that the tower receives 1.78× less power, because the path and direction still need their own terms.
4. Try one controlled change
TryChange only installed antenna gain. Radio output and cable loss stay fixed.
ObserveAt −3.00 dBi, the test port remains 22.5 dBm while EIRP is 20.0 dBm. The gap is 2.50 dB, a 1.78× ratio, and EIRP is 56.2% of the test-port power.
ExplainThe slider cannot change the conducted test because the antenna is outside that measurement plane. It changes only the installed radiated budget.
A dBm comparison is useful only when its reference planes are explicit.
- Conducted
- Cable calibration, connector repeatability, bandwidth, and instrument uncertainty remain
- Radiated
- EIRP is directional and depends on installed pattern, mismatch, efficiency, and polarization
- Coverage
- Tower receive power also needs distance, obstruction, interference, and receiver terms
Pair the conducted result with installed over-the-air and current-trace evidence.
5. Avoid the ratio trap
The 1.78× ratio compares two local budget numbers. It is not a direct ratio of tower receive power, range, packet success, or battery life.
6. Build the lab record
Record reference plane, frequency, bandwidth, calibration date, cable and connector loss, radio setting, uncertainty, enclosure state, antenna match and pattern, orientation, RSRP, SINR, delivery, retries, and current.
7. Check yourself
Why does changing antenna gain not change the test-port output?
What does −3 dBi mean in this example?
Does 20.0 dBm EIRP prove a field pass?
The page compares measurement planes without treating an illustrative antenna loss as measured truth.
- 0.500 dB
- Illustrative cable and connector loss
- −3.00 dBi
- Illustrative installed gain
- 1.78×
- Bench-to-EIRP power ratio only
Go deeper into the chapter's lab gates and approve only the integrated field result.
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