Fibre Optic Loss Budget Calculator
What arrives at the far end of a fibre, and whether the receiver can actually use it — which is two questions, not one. A link can fail because too little power arrives, and it can fail because too much does.
The span
The optics
All three are on the transceiver datasheet. The overload figure is the one people leave out, and it is the one that catches short links.
The budget
The green band is the receiver's usable window. The marker is where this link lands.
How far could it go?
The failure everybody checks for
Too much loss. The signal arrives below the receiver's sensitivity and the link does not come up, or comes up and errors constantly. It is the obvious failure, it is what a loss budget is normally built to avoid, and it is generally caught before anything is installed.
The failure almost nobody checks for
Too little loss.
Every optical receiver has an overload threshold as well as a sensitivity. Above it the photodiode saturates and the eye closes, and the link produces errors. Take a transceiver specified for eighty kilometres, patch it across a rack into an identical unit two metres away, and it can fail immediately — not despite the enormous power margin but because of it.
What makes this expensive is where people look. The sensitivity margin reads 25 or 30 dB, which is wonderful, so power is the first thing ruled out. Hours go into transceivers, patch leads, line cards and configuration before anyone measures the received level and finds it well above the maximum.
The fix is an attenuator, which is counterintuitive enough that it is worth saying plainly: the link needs less signal, not a cleaner one. A 10 dB in-line attenuator in the receive path, costing a few pounds, and the link comes straight up.
What the margin is for
The engineering margin — typically 3 dB — is not padding. It covers things that are certain to happen and cannot be predicted individually:
- Repairs. A cable cut adds two splices. Over twenty years a route through a city will be cut more than once, and each repair is permanent added loss.
- Ageing. Connectors degrade with mating cycles; splices drift slightly; hydrogen ingress raises attenuation in some conditions.
- Measurement uncertainty. The cable's stated attenuation is a specification, not a measurement of your particular drum.
- Later work. A mid-span joint added to serve a new building is loss nobody budgeted for.
A link commissioned with no margin is a link that will fail during its service life, at a time nobody chooses.
Why attenuation depends on wavelength
Two mechanisms, pulling in opposite directions.
Rayleigh scattering falls steeply with wavelength — as the fourth power — because it depends on microscopic density variations frozen into the glass. This dominates at shorter wavelengths and is why 850 nm multimode is an order of magnitude worse than 1550 nm single-mode.
Infrared absorption rises with wavelength as the glass itself begins to absorb. This dominates beyond about 1600 nm.
The minimum sits where the two curves cross, at around 1550 nm, which is why long-haul systems live there and why optical amplifiers were developed for that band rather than another.