I agree that that the pressure is equal everywhere in a static system - like the air in a tire. But in a dynamic system (fluid/air moving under pressure) it has to pass through passages, turn corners, bleed into/through bearings/fittings/etc. Friction is involved as is every change of direction as far as flow/pressure. I swear we did some sort of experiment back in Physics class/hydraulics about this but I don't recall any specifics
However, I readily admit I have never checked an engine for this. Most engines do not have any way to easily attach a pressure gauge to anyplace other than the main oil gallery anyway (except the Norton which has no way to connect it TO the main gallery!) So it may be as you say, the pressure is the same throughout the system.
On the subject of pressure drop in a pipe over distance, I performed some tests a few years back showing how pipe length affects both flow rate from the pipe and pressure drop along the pipe. Thought this information might help clarify some points discussed in this thread regarding the location of an oil pressure gauge in a flowing system. None of the parameters explored here were intended to mimic or address anything related to a Norton motorcycle engine. Nevertheless thought the results had merit as they provide fundamental understanding of pressure and flow in a pipe.
The test rig employed consisted of the following components.
- A metal tank fit with a quick connect inlet that can be pressurized with regulated air pressure
- A valve fit at the tank outlet
- A 0.040” (1 mm) diameter discharge orifice
- Various lengths of 3/16” OD copper line that was interposed between the tank exit and the discharge orifice
- Pressure gauges fit at the air regulator, tank outlet and near the terminal end of the copper line.
Tests were conducted by filling the tank with Amsoil Formula 4-Stroke 0W-40 motor oil and fitting an air line with pressure regulator and gauge to the top of the tank to achieve the desired pressure in the system. The valve was then fully opened which exposed an interior valve area larger than the interior area of the copper tube, thus the valve was not a flow restriction in the system. With the system under full flow, oil pressure was recorded at the tank exit and just ahead of the discharge orifice. Oil flow rate was measured by collecting oil at timed intervals in graduated beakers at the discharge orifice.
In all cases when in the static mode, i.e., with the exit to the system capped off, the air pressure recorded at the regulator, the oil pressure recorded at the tank exit and near the end of the copper tube just upstream of the discharge orifice was identical regardless of the length of copper tubing interposed between the tank and discharge orifice. In contrast, in the dynamic mode, i.e., when oil was being discharged from the system, the moment flow commenced a significant drop in oil pressure was recorded on the gauge near the discharge orifice.
Tests were performed at pressures ranging from ~ 5 to 20 psi, applied to the system via the air pressure regulator attached at the tank inlet. Pressure and flow rate results in the dynamic mode were recorded and are presented graphically below. The results show clearly how pressure and flow rate decrease with increasing pipe length. No revelations here since anybody that has ever used long and short garden hoses has likely made similar qualitative observations. In conclusion, circling back to the subject of Nortons, as others have indicated in this thread, there would be a considerable difference in oil pressure measured directly at the pump output vs at the end of the small plastic line feeding the cylinder head.
There is one more plot related to this endeavor that is not presented here, and that is essentially the same experiment reported here, i.e., oil expelled via a single 0.040” dia discharge orifice, was repeated but with an udder having 3 x 0.040” discharge orifices. As one would expect, the flow rates increased approximately 3X those shown here.
One other interesting aside to this undertaking was realizing that if you have an actual 10 psi pressure acting on motor oil having a viscosity of ~ 20 CSt (the viscosity of 50 weight motor oil at 100C) and being discharged via a 0.040” dia orifice, it will shoot a vertical stream ~ 10 ft in the air where air drag tends to fragment the stream into a spray. That’s an impressive jet of oil coming out of a tiny little 1 mm orifice that is under not very much pressure!