The "ED" abbreviation is new to me, but generally, it is a sort of reverse process, starting with purpose first.
Describing in detail would need a book. And whole books were written on designing steam-engines generally! To summarise though from some of these books:
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First calculate the power needed to accelerate the required loads from rest and maintain them at fair minimum speeds on the steepest gradients. This is a matter of fairly basic Theoretical Mechanics, a branch of Physics; but it does mean having to assess the retarding forces, not just the "ideal" in which the only retarding is that of gravity up a hill. These forces are proportionally a lot lower on a railway than they would be for road vehicles – an observation noted in effect though probably not numerically, on horse-drawn quarry tramways well before the first steam locomotives.
Normally, in British steam-locomotive practice at least, the aim was not to use HP but TE – Tractive Effort, in lbs force. A reciprocating steam-engine's HP and speed in rpm are interlinked; but its mean effective torque (hence a locomotive's pulling-power) is more or less constant for a given admission-pressure and cut-off irrespective of speed.
"Mean Effective" because the torque varies harmonically from 0 at dead-centre to maximum when the crank and connecting-rod are perpendicular to each other, approaching mid-revolution (not mid-stroke). Once the train is well under way the cut-off may have been brought back so early the steam-pressure on the piston is already well below its admission-pressure, at this maximum torque point.
At dead-centres the connecting-rod is simply trying to compress or stretch the crank-arm, and the engine on that side of the locomotive is relying on its companion(s) at other angles, to help it past this stasis. (Single-cylinder traction-engines sometimes need the driver to pull the flywheel round a touch to get them to start.)
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Now design the engine itself (the cylinders and motion) – largely from calculating the theoretical Indicated Horse-Power by the cylinder dimensions and cut-off values to match the specified power and TE as far as possible.
The basic formula for the cylinder alone, in Imperial units, is ePLAN/33000 HP:
P = the Mean Effective Pressure (not boiler or even steam-chest pressure. It is the mean of the pressure-range, of admission pressure to cut-off plus then, that of the hyperbolic expansion to release),
L = Stroke in feet,
A = Area of Piston (square inches)
N= Strokes per minute, which for a double-acting engine is rpm X 2, per cylinder.
and e is a rather empirical decimal fraction called the "Diagram Factor", an efficiency allowance reducing the PLAN product somewhat. It accounts for the internal losses difficult to quantify accurately. They are mainly by temperature cycling, clearance volume and the compression due to the exhaust cut-off / lead-steam cushioning.
That lot gives the result in ft/lb/minute that the 33000 divisor converts to HP. This is the work done only within the cylinder, not that actually between wheel and rail, affected by the intervening frictional losses and the mean torque inherent in a crank-driven transmission.
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From this, derive the steam-raising rate needed, to design the boiler.
This means knowing the thermodynamics: the specific heat and latent heat of water, the calorific value of the coal in BTU / lb, the heat transfer rate from fire to water, superheater variables, steam "losses" to the injector and ejector, and for passenger services, the train heating…
On top of these are conditions such as the low overall thermal efficiency of a steam-locomotive, and the railway's loading-gauge, maximum axle-loadings and minimum curve radii, etc.
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I don't know to what extent the auxiliaries did need considering. On main-line working the small ejector is on continuously, and the injector on at least for much of the journey. The larger BR Standards and similar also have exhaust-steam injectors that lessen their boiler-steam draw a bit though still need an auxiliary live-steam feed: a steam-relay valve brings in more from the boiler when the driver closes the regulator. In full size the injectors were designed to meet steady mean water demand though; unlike the intermittent use more familiar to most of our miniatures with injectors matched to boiler size more than steam use. In Winter the train-heating would have been on continually. However. by far the greatest drain on efficiency is the loss of heat directly up the chimney, followed by radiation despite the cladding.
It is worth bearing in mind though what the official training-manuals issued to railwaymen said about steam-demand and firing rate: that these average to be fairly constant throughout most of the journey.
Edited By Nigel Graham 2 on 24/05/2023 11:10:20