Theory and Stuff, yet again….
 
 
  THE STEAM 
  POWER 
  CYCLE, 
  a brief 
  overview.
 
 
  EXPANSION in terms of the Rankine Cycle is the process whereby steam expanding to lower 
  temperature and pressure exerts force against a piston or turbine blade which then converts that force 
  into work.
  A piston steam engine is either expanding or non-expanding, depending on whether the steam is 
  “cutoff” at some point in the piston travel or is admitted throughout the full stroke.  Expanding engines 
  are proportionately less powerful because the pressure diminishes during the stroke, the exhaust steam 
  having very little available energy remaining to perform work.  Non-expanding engines are 
  proportionately more powerful but much less efficient, the exhaust steam having much available energy 
  still remaining when leaving the cylinder.  Because economy is an important aspect of automobile 
  engineering, we will confine our discussion to expanding engines.
  Cutoff is expressed as a percentage of the stroke, if the valve closes ¼ of the way down the cylinder we 
  refer to it as a 25% cutoff.  A more useful measurement is the expansion ratio, the ratio of the volume of 
  steam in an engine cylinder or turbine when the piston is at the end of the stroke to the volume at cut-
  off. 
  The “clearance volume”, which is the volume between the top of the piston and the cylinder head when 
  the piston is at the most upwards position, must be established to determine the expansion ratio.
  Given the engine cutoff of 25% (above), the change in volume in the cylinder will equal the volume 
  uncovered by the piston between the upper most point in its travel (called top dead center or TDC) and 
  the cutoff at 25% of the piston stroke.   Let us also assume the clearance volume equals 25% of the 
  cylinder volume uncovered throughout a full piston stroke.  The cylinder volume at cutoff is equal to 
  the clearance volume plus the cutoff volume.  The total cylinder volume at the bottom of the stroke 
  (BDC) equals the volume uncovered by the piston plus the clearance volume.
  The expansion ratio will be:  
  Total cylinder volume at BDC / cylinder volume at cutoff
  The cylinder volume equals the volume at BDC, or 100% of the stroke volume, plus the 25% clearance 
  volume, or 125%.  The volume at cutoff equals the cutoff of 25% plus the 25% clearance, or 50%.  
  125% / 50% = 2.5 to 1
  Increasing steam expansion also tends to increase engine efficiency; less pressure leaves the engine by 
  way of the exhaust and is instead absorbed by the piston to do work. Eventually, the pressure drops to a 
  point where the work produced is less than the engine back pressure and friction, indicating very 
  practical limits to the amount of practical expansion. 
  Steam temperature also influences power and economy.  Temperature falls along with pressure during 
  expansion; since saturated steam is at the condensation temperature, even a little expansion removes 
  enough heat to cause a portion of the steam to condense.  Water occupies far less volume than the same 
  weight of steam and such condensation causes an accelerated drop in the cylinder pressure with an 
  accompanying fall off in work performed.   Increasing the temperature above the saturation point 
  produces superheated steam which is able to expand further and produce more power before the onset 
  of condensation.  The sensible heat required to produce superheat is small compared to the latent heat 
  of vaporization and thus the added work from superheating is significantly greater than the energy 
  used to add the superheat initially.
 
 
  Steam enters at 500 psi in both cases, with a cutoff of 30% in the upper graph with a cut off at 30%
  and 5% in the lower. The curves represent the pressure as the piston travels down the cylinder, 
  with the area beneath the curves being equal to the work developed.  The average pressure for the 
  stroke in the upper case is 320 psi and 84 psi in the lower.  We can say the Mean Effective Pressures 
  were 320 psi and 84 psi, respectively, and estimate that in the second case the engine is about 
  one-fourth as powerful according to PLAN.
 
 
  “Mean Effective Pressure”, (MEP), the average steam pressure during an engine stroke, is proportional 
  to the power developed and generally inversely proportional to efficiency.
  These graphs reflect the same engine running with the same steam pressure, but with using differing 
  cutoff:
 
 
  Because 19th century steam engine valves 
  usually admitted and exhausted steam 
  through the same port, the hot incoming 
  steam traversed a passage just travelled by 
  the outgoing cool exhaust, cooling the 
  incoming steam and causing premature 
  condensation, robbing efficiency.  Breaking 
  the expansion into smaller steps reduces 
  the temperature drop in each cylinder, less 
  heat is transferred to the engine parts, leading 
  to a further efficiency gain.  “Compounding” is 
  the process of breaking expansion into smaller 
  steps and to this day is the basis for our most 
  efficient and advanced steam and gas turbines.  
  Each expanding element is now termed a “stage”, 
  though at one time it was called an “expansion”; 
  thus an engine that expands the steam three 
  times is a triple expansion engine or a three-stage 
  expander.  An expander with just one stage is 
  a “simple” expander and two stages a compound.
  The drawing to the left illustrates the basic 
  components of a compound engine.  The 
  smaller high pressure (HP) cylinder, to right, 
  partially expands steam which exhausts to a 
  receiver.  The receiver levels out variations in 
  pressure and supplies steam to the larger 
  low-pressure cylinder (LP) which expands the 
  steam further.  By adding stages, one can 
  accommodate higher steam pressures and 
  shorter cutoffs.
 
 
  PLAN is an acronym for a formula to calculate theoretical horsepower in a single cylinder:
  Pressure
  (MEP, in psi)
  Length
  (of stroke, in feet)
  Area
  (cylinder inside diameter, square inches)
  Number
  (of revolutions, per minute)
  Horsepower = (P x L x A x N) /  33,000
  We can verify this equation by comparing it with basic terms in mechanics, the first being that 1 
  Horsepower = 33,000 foot-pounds per minute.   
  *
  The Pressure (MEP) multiplied by the piston area determines the average force on the 
  piston in pounds.
  *
  The distance the piston travels in feet multiplied by the average force in pounds yields the 
  work produced in foot-pounds.
  *
  The work produced times the number of RPM calculates the power developed per minute 
  in foot-pounds per minute.
  *
  Dividing the power by 33,000 converts the work from foot-pounds per minute to 
  horsepower.
  The area beneath the upper curve looks relatively ‘fat’ compared the relatively, ‘skinny’ lower 
  curve; engineers study such curves to determine both potential power and efficiency.  Fat curves, 
  with their higher MEP, produce more horsepower for their size but do so by wastefully disposing 
  pressurized steam from the exhaust.  Skinny curves indicate the steam is fully expanded and 
  operating efficiency but also indicates lower overall power output.  Mechanisms called valve gears 
  regulate how early or late in the stroke cutoff occurs, adjustable valve gears can provide either 
  skinny or fat curves as needed.
  Short cutoff implies the valve will be open briefly, which in turn requires high valve speed to 
  complete the cycle from closed to open and closed again in a short time; such fast operation is 
  technically demanding as extra stress, friction and wear must be managed. Overall efficiency 
  improves with the adoption of higher pressures and temperatures, if the engine can expand the 
  steam fully. The inability to use short cutoff practically limits useable pressures and efficiency.  In 
  the 19th century it became feasible to generate higher steam pressures, but remained a challenge to 
  build valves able to use the steam effectively.  Suppose we desire a cutoff of 10%, but can only 
  practically build engines of 30%, it soon becomes apparent that the steam leaving the cylinder still 
  possesses enough pressure to operate another cylinder.  By expanding transferring this exhaust 
  steam to a larger cylinder and cutting it off at 30% cutoff, transferring the steam to a larger 
  cylinder and expanding again with 30% cutoff, we achieve a higher overall expansion ratio than 
  our desired 10% cutoff.  Rising pressures and temperatures led to the use of three and even four 
  cylinders.
 
  
  
  
  
 
   
 
 
   
 
 
   
 
 
  