by Iver P. Cooper
There were some tidbits which I couldn’t fit into the main article Saddling the Iron Horse published in Grantville Gazette 7, but I thought I should preserve for reference purposes.
I have grouped the information according to the headings in the Iron Horse article. Please note that this Addendum is going to seem very disjointed to anyone who has not read the main article recently.
1. Railroading in 1632 Canon
In Elizabeth, Ken Hobbs mentions that there was abandoned main line track in the middle of town, which was just paved over. This, he implied, could be salvaged–of course, at the cost of damaging asphalt roads in a world in which asphalt is relatively hard to come by.
More particulars on the Grantville-Halle line: “On a cold spring morning in 1634 a new train was loading up in Grantville to move north…. Another difference was the load on this train was made up of steel-wheeled railcars, not rubber tired vehicles. These trains were loaded on the standard gauge flatcars for transport to Halle, where they would be loaded on barges.” (Elizabeth).
2. Grantville Railroading Knowledge
2.1. Several children’s books, which may be in personal libraries in Grantville, are surprisingly informative.
Weitzman, Locomotive: Building an Eight-Wheeler (1999) is set in 1870 and describes the drafting stage, factory equipment (engine, drill press, lathe, planer, steam hammer, overhead crane), and various process steps (cutting, rolling, hole punching and riveting the sheets to make boilers; molding the bell, erecting the locomotive, and hand-finishing the parts so they fit together). The locomotive, a wood burner, is said to have taken eight weeks to construct, and to have 72 inch cast iron drivers, a boiler pressure of 12 p.s.i., and 3,000-pound cylinders.
Johnstone, Look Inside Cross-Sections: Trains (1995) depicts an American 4-4-0, using an exploded view, and notes that in 1870, 85% of U.S. locomotives had that wheel arrangement. The most interesting features depicted are the lead bogie truck (with one axle and wheel omitted), and the boiler flue tubes (I counted 109).
On the drawing of a 4-12-2, you can spot an equalizing lever over the drivers. Page 18 notes that “like most steam locomotives, the 4-12-2 was fitted with an arch made of fireproof bricks at the front of the firebox. It acted as a baffle to make the coals burn at maximum heat and cut down the quantity of smoke produced.” Johnstone also notes that the front and rear driver had sideplay, enabling the 4-12-2 to negotiate a 16 degree curve.
The 4-12-2 is said to have three cylinders (27×32, 27×31), 67 inch drivers, a weight of 202 tons, a top working speed of 60 mph, and a wheelbase of 52’3″.
There are also depictions of Pacifics (4-6-2) and a rack loco.
2.2. While there are no steam locomotives in Grantville, we can find other useful equipment. For example, the West Augusta Historical Society in Mannington, West Virginia apparently has a “captive caboose,” designation “B&O C2283”, which is a Class I-5d. That means that we have the opportunity to examine up-time couplers, brake, and wheels. The Society has other artifacts from the heyday of railroading in Mannington.
Others have no doubt been collected by rail fans.
Jeffrey S. Ward, Sr. explained on the Atlas forum that over the decades, B&O operators on the branch lines in the area “would have been glad for somebody to talk to, and would probably have been pretty loose with timetables, train orders, and other assorted railroad paraphernalia,” and thus the local rail fans would have been able to pick up a fair amount of “railroadiana” in flea markets.
A search of attics and basements might also produced unexpected marvels; perhaps a former resident worked on the railroad, and left memorabilia behind.
Of the probable finds, the most useful would be rulebooks, textbooks, and tools.
2.3. By way of guidance as to what a Grantville railfan might have, Trynn Allen (on the Atlas forum) noted that his personal library comprised “about two dozen issues of Model Railroader, three books on engines, two books with lots of pictures of engines and rolling stock, and the models themselves.”
2.4. One book I really hope the up-timers have in Grantville is Comstock’s The Iron Horse (which I found at the Fairfax County Public Library). Its felicities include illustrations, with discussion, of the parts of a steam locomotive (front endplate), Jervis’ three point suspension (39), locomotive stack designs (45), reversing mechanisms (46), the Bury firebox (54), Miller’s traction increasing levers (62), Harrison’s equalizing levers (66), Baldwin’s flexible beam truck (74), sand domes (88-9), wagon-top boilers (102), an exploded view of The General (104-5), a double-ended locomotive (108), a swiveling engine unit (109), the Stephenson valve gear (110), the Walschaerts valve gear (111), the first Westinghouse air brake (125), pumps to increase draft (127), a firebox with a brick arch (129), Shay, Heisler and Climax geared locomotives (158-9), thermic siphons (194), water circulators (195), and an exploded view of a “Big Boy” (back endplate). There is a lot more here, too. For example, Comstock notes that the three-point suspension system made it possible for the seven ton John Bull to run on metal-surfaced wooden rails (38-9), and explains the problems encountered with water tube fireboxes (182).
2.5. While the main article only cites the 1911 Encyclopedia Britannica, and its modern counterpart, the enthusiastic efforts of encyclopedia salesmen pretty much guarantees that there are editions from the eighties, seventies, sixties, fifties and forties in homes in Grantville. They were probably purchased when the kids were in middle school or high school. The old encyclopedias may lie forgotten in an attic or basement, but they are there. I saw a 1955 set being given away at a library, and looked at the locomotive entry. While the article gave more space to diesel-electrics, it had a respectable amount of material on steam locomotives. This included some very detailed views of a Pacific 4-6-2 locomotive, with cab, firebox, boiler, drive wheel, cylinder and smokebox details. An encyclopedia from the forties or thirties, when steam was still dominant, would no doubt be even more helpful.
3. Motive Power
3.1. The smallest of the Vulcan gasoline locomotives listed by Connor weighs four tons, has a 25 horsepower engine, sixteen inch diameter drivers, and a rated drawbar pull of 1,600 pounds. Thus, if the train resistance per ton is ten pounds, then the locomotive can haul 156 tons of cargo, probably at about 5 mph. The largest locomotive in the table weighs fifteen tons, has a ninety horsepower engine, twenty-five inch drivers, and a rated drawbar pull of 6,000 pounds. So it can haul, under the same rail conditions, 585 tons of freight.
3.2. It is also possible to power a locomotive from a central station. The latter generates electricity and transmits it to the locomotive, which uses it to power electric motors which turn its wheels. While these electric locomotives are used in modern high speed transit systems, they require an extremely expensive infrastructure (the central station, electrified rails or overhead lines, etc.). Right now, we have to focus on what is feasible with the USE’s present resources, which are stretched thin by the war. Steam locomotion seems the best approach.
3.3. In steam-electric locomotives, the steam engine drives an alternator or generator, which in turn powers an electric motor which drives the axles. The advantage is the elimination of the reciprocating rods; the disadvantage is the inefficiency of the energy conversion. There have also been a few steam-turbine locomotives.
3.4. Diesel-electric locomotives (in which the diesel engines power electric motors) have low operating costs, but high initial costs–perhaps five times that of a steam locomotive of equal horsepower. (NOCK/RE 203).
3.5. According to Douglas Jones (private communication), “Natural gas conversion may be used locally around Grantville. This is canon for the trolley system, but if I was using a pickup truck as an engine locally, I’d use a natural gas converted gasoline engine. These will need regular refills. Rubber and plastic hose is not safe for use with methane (it suffers from methane embrittlement and has a working life of only a few months at pressure), so they’ll have real problems refilling high pressure portable methane tanks from fixed compressor stations. There will probably be corrugated stainless steel gas piping (the kind used to plumb natural gas into houses) that they can use, to a limited extent. The total supply of such pipe will probably be only a few tens of yards. Common air compressors will work just fine to compress the methane.”
4.1. Fuel Efficiency. One pound of good coal yields about 15,000 British Thermal Units (BTUs) heat energy, of which 50-80% is transferred to the water. When the steam is released from the steam dome into the cylinders, about 7-11% actually does work (i.e., moves the pistons), and the rest escapes. So the overall thermal efficiency is only about 6% (900 BTU per pound of coal). (EB11)
4.2. Exotic Fuels. In theory, it is also possible to burn natural gas, or crude biomass such as peat, rapeseed, hemp, corn, sawdust or sugarcane waste. However, these possibilities are best explored after we relearned how to build a more-or-less traditional locomotive.
4.3. In terms of heating capacity, the general rule is that 2,000 pounds of coal is equivalent to 5,250 pounds (1.75 cords) of wood.
4.4. The American Far West was coal-poor, so railroads in that area were eager to switch to oil burning after the big California oil strikes.
4.5. Another good reference on the subject of coal quality is Anonymous,”Australian Coal,”
5. Engineering Design 101
6. Steam Locomotion
7. Basic Train Resistance to Motion (Straight, Level Track)
7.1. EB11 formulae contemplate speeds of 37-77, or even 47-77, mph, which may be a trifle fast for the first few years of the USE rail system. USE engineers may therefore need to determine the appropriate formulae for their rail operations by putting a “dynamometer car” between engine and the train, and measuring the drawbar pull at different speeds.
7.2. Physicists teach that rolling friction is inversely proportional to wheel diameter [cite]. However, in practice, wheel diameter doesn’t have much effect on train resistance. I believe that this is because rolling friction is only one of many factors contributing to train resistance.
7.3. Initially, to get a train moving, you need about twenty pounds of force for every ton of load. Fortunately, because of coupling slack, the locomotive only needs to start one car at a time.
Starting resistance is to overcome friction with the wheel bearings, and is higher (25-30) for journal bearings than for roller bearings (5-15)(AREMA). Once the train is actually moving, the “basic resistance” is much lower.
7.4. The train “punches a hole” in the air, so the locomotive encounters much more air resistance than do the cars it is hauling.
8. Extra Train Resistance (Grades and Curves)
8.1. The locomotive must be given sufficient tractive force to haul the expected load over the “ruling grade” of the track. The first “mountain railway” in Germany (Windbergbahn, 1856) had a gradient of 2% (steep by modern standards), but even higher gradients were occasionally tolerated on main lines in early nineteenth century America (e.g., 5% at Kingwood Tunnel on the original B&O).
8.2. The sharper the curve, the greater the problems presented. (Armstrong, 26). Sharpness can be expressed as 1) the angle through which the track turns in 100 feet, say, one degree, or as the radius of the circle corresponding to the curve (for a one degree curve, it is 5,729 feet). The Windbergbahn had a twenty degree (286 feet radius) curve.
When a train goes around a curve, centrifugal force causes its wheel flanges to grind against the rail. This creates curve resistance.
It also cause the train to tip outward. Depending on the exact design of the track, a train on a curve might have to slow down to avoid derailing. The speed on a fifteen degree curve might be half that on a five degree one, and one-quarter that on a mild one degree veer.
As it comes out of the turn, the train must accelerate to regain its former speed.
8.3. You need extra tractive force (above and beyond that needed to overcome the base train resistance) whenever you want to accelerate; as Newton said, Force equals mass times acceleration. According to EB11, the acceleration resistance equals the weight of the train, multiplied by the ratio of the desired acceleration to gravitational acceleration.
9. Rated Tractive Force
9.1. To achieve the maximum traction, the engine would need to have appropriately sized cylinders, piston rods and wheels, and the boiler needs to generate sufficient pressure in the cylinders.
9.2. The mean effective pressure in the cylinder is a function of the actual boiler pressure, and the “cutoff”; steam is admitted only for part of the stroke; and then is just allowed to expand against the piston. A long cutoff is used when you want to start the train, or pull an especially heavy load. A short cutoff is more economical. For starting the train, the cutoff is typically such that the mean effective pressure is about 85% of the boiler pressure.
9.3. Even when you have a full head of steam, there is no point in admitting steam into the cylinder for the entire stroke. That is because the steam does work only when the crank is not parallel to the main rod. (Maximum work is done when the crank is at right angles to the main rod.) For the remainder of the stroke, the steam expands and the cylinder pressure drops accordingly. So the cylinder pressure, averaged over the entire stroke, is less than the actual boiler pressure. See http://www.railway-technical.com/st-vs-de.html
9.4. Even with a long cutoff, the boiler pressure drops below the nominal value if you increase the piston speed, and the boiler can’t keep pace with the demand for steam. Hence, it is customary for the cutoff to be reduced when speed is increased, so that the steam demand is sustainable. Reducing the cutoff naturally also reduces the mean effective pressure.
9.5. The standard value 0.85 is apparently a compromise value representing the effect of steaming capacity on mean effective pressure. One online source quotes a classic text (Hay’s Railroad Engineering, 1953) as giving the following dependence of mean effective pressure on locomotive speed:
|Speed (mph)||Proportion of Rated Tractive Effort Available|
See this fairly complete technical discussion.
Note that 0.85 corresponds to a speed in the 20-30 mph range.
9.6. Other sources express mean effective pressure as a function of piston speed. Connor (88) says that the mean effective pressure is 42.5% of boiler pressure at a piston speed of 750 feet/minute, 30% at 1,075, and 22% at 1,500.
9.7. A table in the Baldwin Locomotive Company catalogue assumes that the longest cutoff is such that the mean effective pressure is no higher than 85% of the boiler pressure. I have studied the various trend lines to deduce the underlying formula relating the mean effective pressure to the locomotive speed and a measure of steaming capacity (the ratio of rated tractive force in pounds to heating area in square feet). Above a speed equal to 120/ratio (e.g., 12 mph for the typical American, ratio 10, the MEP as a percentage of nominal boiler pressure is
0.85 * 15,000 /(speed mph * ratio)
So, if speed 30 mph, and ratio is 10
For lower speeds, the mean effective pressure, as a percentage of boiler pressure, is
0.85-(.000354*ratio*speed) * 100
So at 10 mph, with ratio 10, the MEP is about 81.5% of the boiler pressure.
The same catalog also says that the rate of supply of steam is only just adequate for the desired engine power when there is one horsepower for each 2.5 square feet of heating area.
10. Maximum (Adhesion-Limited) Tractive Force
10.1. If the rolling friction is so small (a few pounds per ton of load), why is the coefficient of adhesion so high (400-500 pounds per ton of locomotive)? In essence, we are looking at the difference between rolling friction, and sliding friction. The coefficient of adhesion is actually measuring the tendency of the locomotive to slip, and that is related to sliding friction rather than rolling friction. With many surfaces, it requires much less force to roll than to slide.
For steel on steel, the coefficient of rolling friction is [insert], while that of sliding friction is [insert] (static, i.e., from rest) or [insert] (dynamic, i.e., if you are already moving).
11. Weight and Size
11.1. Clarke (121) simply says that ordinarily no more than 12,000 to 16,000 pounds should be placed on a wheel.
11.2. The more driving wheels a locomotive has, the greater the length of its wheelbase. The maximum rigid wheelbase which can negotiate a curve is proportional to the square root of the radius of the curve. (Profillidis, 237)
11.3. The practical limit for non-articulated locos running on normal track is probably twelve coupled driving wheels, and even those were rare. The only fourteen-coupled locomotive ever built was the Soviet AA20. According to Doug Self, “It was clear (though never publicly admitted) that the AA20 was a complete disaster. It spread the track, wrecked every set of points it passed over, and derailed almost every time it moved. Steaming was poor and the locomotive too powerful for existing couplers and too long for the turntables. After 1935, it was stored for 25 years at the Shcherbinka test facility and finally scrapped in 1960.”
11.3. On the issue of loading gauge, Douglas Jones commented, “The few existing rail cars within the Ring of Fire (has anyone got an inventory of these — a flatcar here or a boxcar there) may force the issue by being built in conformance to the North American loading gauge. Other equipment will be built to match.”
11.4. With respect to mismatch between car width and track gauge, Douglas Jones has told me, “2 foot gauge railroads in Maine used equipment that was 6 feet wide. The WW&F railroad has drawings of some of their cars on their web site.”
12. Making Steam: Locomotive Boiler Design
12.1. The best illustration I have seen of the brick arch and deflector plate is on page 21 of Tufnell, The New Illustrated Encyclopedia of Railways (2000). It also has a coherent description of three-point suspension on page 20 (see also 73).
Unfortunately, that is too late to have been passed down through the RoF.
12.2. EB11 doesn’t have any teachings as to a preferred tube length, but you could probably estimate it by comparing boiler length to wheelbase for selected locomotives in the Alexander book. More educated guesswork is needed to arrive at the number of tubes, and their diameters.
12.3. Kinney (see refs) has a nice study of the internals of a 1880s-1920s locomotive boiler.
13. Putting Steam To Work: Locomotive Engine Design
13.1. The maximum piston acceleration (feet/sec^2) is ((W^2 * S)/2189) * (1 + (1/(2*N)), where W is drive wheel speed (rpm), S is piston stroke length (inches), and N is the ratio of the main rod length to the stroke length.
14. Cranking the Wheels: Locomotive Transmission Design
14.1. Adding additional weight to the counterbalance, beyond that needed to balance the rotating masses, is called overbalance. The overbalance transforms the horizontal imbalance created by the reciprocating parts into a vertical imbalance. The latter causes hammer blow on the rails. Ludy 100 says that the hammer blow is proportional to the overbalance mass, and to the square of its rotational velocity about the center of the wheel.
More detailed analyses are available online. According to Rai University, Theory of Machines II, Lessons 16-19, if R is the mass of the reciprocating parts (piston, crosshead, etc.), then the force needed to accelerate them in accordance with a simple crank and connecting rod arrangement is R times
W^2*r*(cos theta + (cos (2*theta)/n),
where W is the angular speed (radians per second) of the crank, r is the length of the crank, n is the ratio of the length of the connecting rod to the length of the crank, and theta is the crank angle (radians). The first part is called the primary force and the second is the secondary force.
Thanks to Newton’s Third Law, the force accelerating the reciprocating parts elicits an equal but opposing force (the inertia force) on the rest of the locomotive.
The inertia force varies with the crank angle, and if unbalanced, this creates “horizontal” shaking (i.e., along the line of reciprocation). That shaking, please note, is proportional to the square of the wheel speed. An unbalanced horizontal inertial force creates a variation in tractive force, and swaying.
If the horizontal force is balanced by a weight mounted on the wheel, the balancing weight itself creates an unbalanced vertical inertial force, the latter creates hammering on the rails, alternating with lifting of the wheel off the rail. (This is euphemistically called “dynamic augment”.)
The variation in tractive force and the swaying are proportional to 1) the unbalanced portion of the reciprocating weight, 2) the crank radius (which is half the stroke length), and 3) the square of the crank (wheel) speed.
Likewise, the alternating hammer blow down on the rails, and the lift up from the rails, are proportional to 1) the overbalance weight, 2) the radius at which the counterbalance is placed, and 3) the square of the wheel speed.
Thus, the locomotive cannot be allowed to travel with a wheel speed higher than the square root of: the weight on the wheel, divided by the product of the horizontally balanced reciprocating weight and the counterbalance radius.
The crescent-shaped counterbalance is placed on the wheel as far as possible from the center of the axle (Ludy, 100), so the counterbalance radius is nearly equal to the wheel radius.
It can be proven that the “resultant” (vector combination) of the horizontal and vertical unbalanced forces is smallest when the half the reciprocating mass is balanced by the wheel-mounted counterbalance. However, when the track is light, one may deliberately balance less than half, or in special cases, none at all. (Self, Balanced Locomotives)
14.2. The need for counterbalance, and thus the amount of hammering, is reduced if the locomotive has a second pair of pistons, so that, on each side of the locomotive, one piston is moving forward while the other is moving back. The engine parts can then be made lighter, too, since four cylinders share the work of driving the wheels. (Self; Sinclair 491-3, 692; Alexander PL75). Several four-piston locomotives were introduced, but the approach never won widespread acceptance, because of the additional mechanical complexity.
15. Rolling Forward: Locomotive Wheel Design
15.1. Reducing the wheel size increases the forces acting on the connecting rods, making them more liable to failure (Forney).
16. Locomotive Wheel Arrangements
16.1. Tufnell says (190) that over 24,000 4-4-0s were built in the US. Late model 4-4-0 PaRR Class L 1890: 18,5 x 26 cylinders, 90 inch drivers, 200 p.s.i. boiler, 1900 ft2 heating area, 32 ft2 grate, 134,505 lb weight, tractive force 18,900 lb, indicated horsepower of 660 at 70 mph. (191)
17. Puffing Away: Locomotive Smokebox Design
17.1. One pound of coal requires about twenty pounds of air to burn properly (EB11).
18.1. Speed, as noted in the main text, is a function of both drive wheel diameter and piston speed. Specifically, speed (mph) is .01785 times drive wheel diameter (inches), times average piston speed (feet/minute), divided by stroke length (inches). The drive wheel speed (rpm) is six times the piston speed, divided by the stroke length.
Note that the greater the stroke length, the faster the piston must move in order to achieve the desired rpm or locomotive speed.
18.2. In the early 1900s, Baldwin Locomotives recommended a maximum piston speed of 1,600 feet/minute, and an “economical” one of about 1,100.
18.3. Maximum Speed. A model railroading site says,
“A steam locomotive’s top speed capability in mph is normally around the same as the diameter of the driving wheels in inches…. In fact any driving wheel rotating at 336 rpm will be running at a speed equal to the diameter in inches. This is called the “diameter-speed.” http://www.ogauge.co.uk/motors.html
At 336 rpm, the piston speed (feet/min) is 56 times the stroke length (inches). So a twenty inch stroke would imply a piston speed of 1,120 feet/minute.
A more complex rule of thumb is
latter 19C, use 0.75 X driver diameter
~1900, use 1.0 X driver diameter
1910, use 1.25 X driver diameter
end of steam, use 1.6 X driver diameter
What is going on here is that changes in materials technology made possible higher driver RPMs.
The designers of a 21C steam loco (5AT) use 1.5 times driver diameter as the estimate for the maximum speed. [5AT]
19.1. For a given engine design, there is a piston speed for which the power is a maximum (EB11).
19.2. Armstrong (43) says that “a 3,000-hp locomotive can move more than 5,000 tons at 30 mph on level track.” [Note that by the Baldwin formula, the rolling resistance is 8 pounds per ton, so 5,000 tons implies a need for 40,000 pounds of tractive force, and use of 4,000 horsepower. Armstrong uses the Davis formula, according to which a loaded 125 ton, 4 axle roller bearing car has a rolling resistance of 4 pounds per ton at 30 mph, see p. 19. 5,000 tons at 30 mph then would only need 2,000 hp.]
19.3. EB11 says that “the maximum power which can be developed by a locomotive depends on the maximum rate of fuel combustion which can be maintained per square foot of grate.” This isn’t really true, it depends on the maximum rate of steam generation (water evaporation), which can correspond to a lower rate of fuel combustion.
20. The Steam Balance
20.1. The ratio of rated tractive force (pounds) to total heating area (square feet) is a useful measure of the relationship of the engine’s maximum steam demand to its ability to supply steam. This assumes, of course, that there is an adequate grate area. The usual ratio for different locomotive designs is given in an early 20C Baldwin Locomotives catalog.
Atlantic (4-4-2) type, 8
Pacific (4-6-2) type, 9
American (4-4-0) type, 10
Mikado (2-8-2) type, 10
Ten-wheeled (4-6-0) type, 11
Consolidation (2-8-0) type, 14
Switching Locomotives, 16
21. Coaling Up
22. Locomotive Design: Putting It All Together
22.1. Connor (91) says that a freight locomotive should have an average speed of 15 mph when hauling 80% of its maximum load.
22.2. A piston rod is essentially a cylindrical column which gets compressed and stretched. There will be a critical compressive force which causes the rod to buckle, and it will be proportional to (1) the modulus of elasticity (which is characteristic of the particular material), and (2) the area moment of inertia (itself proportional to the fourth power of the radius of the cylinder), and inversely proportional to the square of the length (height) of the rod (column). So if you double the length, then, to keep the critical force constant, you need to increase the radius by 41.4%. The mass of the piston rod is proportional to the length times the square of the radius, so this will quadruple the mass.
If you double the boiler pressure, you double the force on the piston, and you need to increase the radius to compensate. the rod mass will increase by 41.4%.
If you double the cylinder diameter, you quadruple the force, and you need to increase the radius once again, this time enough to double the mass.
The partial balancing of these increased reciprocating masses will naturally result in a corresponding increase in hammer blow and a decrease in the safe operating wheel speed.
23. Geared Locomotives
23.1. Douglas Jones says, “Geared locomotives were used on mountain mining railroads, for example, the 2′ gauge Gilpin Tramway in and around Central City, Colorado. The Georgetown loop in Colorado also used Shays, as did the Argentine Central line up to the continental divide from Silver Plume. These lines were 3′ gauge.”
23.2. To compute the tractive effort of a geared locomotive, use the standard formula, but in place of the true driving wheel diameter, use that number divided by the gear ratio. So a Shay with forty inch wheels and a 2:1 gear down will have the tractive effort of a rod locomotive with the same cylinder diameter, stroke length and boiler pressure, but with twenty inch wheels. (Riedel)
24. Second Generation Locomotive Concepts
25. Other Locomotive Design Features
25.1. More on headlights: “Kerosene lanterns were commonly used in early locomotive headlights. They need glass chimneys, and they need glass, both for the lens in front of the lamp (to keep the wind out) and for the mirror behind the lamp. Until they can get the glass for these, nighttime operation will rely on salvaged automotive headlamps and batteries, unless they put steam-powered generators on the engines (automotive alternators with turbines work just fine).” (Douglas Jones)
25.2. More on cowcatchers: “Even European locomotives that live their entire lives between fences have steel bars hanging down to just above the rail in front of the lead wheels. These are there to knock aside rocks or tree branches that might fall on the rail. Without them, the train would have to run at a crawl after each wind storm so that the crew could clear the tracks of any debris that could threaten the train. Also, of course, the pilot (modern term for the cow catcher) can easily be shaped so that it will plow through a light snow. Northern north American and European practice is frequently to build permanent snow plows into the pilots of most engines.” (Douglas Jones)
25.3. More on sanders: “Even very small electric mine locomotives had sanders, these are essential when the track is damp and even more important is there is clay-ey mud in the area.” (Douglas Jones)
25.4. Lubricators. Lubrication will initially be manual, with animal fat. Once oil is readily available, it will replace animal fat, as it will have a greater operating temperature range. Eventually, mechanical or hydraulic lubricators will be used to reduce wear, e.g., between piston and cylinder, or on flanges when taking a curve. Note that superheating cannot be fully exploited until the cylinder lubricants are able to tolerate the higher temperature steam.
25.5. Roller bearings. These reduce friction. (AREMA; Sinclair 688). However, Grantville is likely to first make journal bearings out of Babbitt metal.
25.6. More on water quality: EB11 “Boiler” 148 discusses methods of softening feed water.
Cleaning a locomotive boiler, with its many narrow tubes, can require heroic measures. “You build up a full head of steam, then open the “blow down” valve on the bottom of the boiler…. The rapid depressurization leads to massive foaming inside the boiler; this cracks loose boiler scale and suspends the “boiler mud” that has accumulated at the bottom of the boilers. Since this mud is heavier than water and since the blow-down valve is at the bottom, blowing down the boiler gets rid of a good part of this mud. Steam engines are routinely blown down several times a day where the water is hard. It’s an impressive operation, and you definitely do it where there’s nothing of value trackside,” as that is where the steam is blasted. (Douglas Jones)
25.7. Water scooping. It is also possible for water to be deposited in a trough, between the rails, and scooped out as the train passes overhead. (Nock/RE, 150; Alexander PL55). The train has to be running at high speed for this to work, and it is needed only on long nonstop runs, so it is not likely to be a feature of the first decade of post-RoF railroading.
25.8 More on Tank Locomotives: At least five tank locomotives are depicted by Alexander (PL62, 70, 76, 83, 92). The 1891 model, a 0-10-0 freight locomotive (PL83), carried 3 tons of hard coal and 1,800 gallons of water. Trailing wheels may be desirable in a tank locomotive, to support the storage section; three of the four tank designs shown by Alexander have trailing wheels.
It should be noted that a tank locomotive can be accompanied by a tender for extended range. Or it can haul coal hoppers and water tankers, and dip into them when necessary.
25.9. Flangeless wheels can slip completely off the track, and consequently railroads operating locomotive with flangeless drivers may lay a guide rail on the inside of a tight curve to keep this from happening.
25.10. There is a cryptic reference to “equalizing levers” in Alexander’s plate 72. Unlike some equalizing levers, these allowed the weight distribution between the driving and trailing wheels to be changed. That way, you could have a lot of weight on the driving wheels when you were trying to start the train, and then shift some of it off in order to get a smoother ride.
25.10. More on water supply. The 1830s John Bull used a pipe with a flexible leather sleeve to transport water from the tender (more precisely, from a barrel on the tender), to the boiler. (Comstock, 42). So this shows that leather can be used for flexible connections, prior to the advent of rubber hoses.
26. New Topics
This is where I address topics that didn’t fit into the Iron Horse article, but are still of interest.
26.1. Locomotive construction. There are several good sources of information on how one actually would construct a steam locomotive. I already mentioned the Weitzman book. Another is “How a locomotive is built” (1907)
26.2. Cog locomotives. These can climb even steeper grades than can a geared locomotive, but since they require a specialized track (with a toothed rack), they have been relegated to a future article on the railroad network. For a quick overview, see en.wikipedia.org/wiki/Cog_railway
27. Additional Sources
Comstock, The Iron Horse: America’s Steam Locomotives: A Pictorial History (1971).
Profillidis, Railway Engineering (1995)
[NOCK/D] Nock, The Dawn of World Railways 1800-1850 (1972)
[NOCK/L] Nock, Locomotion: A World Survey of Railway Traction (1975).
Kinney, “Anatomy of a antique traction engine boiler (locomotive style.),” http://www.herculesengines.com/Steam/Boiler%20Construction/index.htm
“Japanese Steam Locomotive Data,” http://www008.upp.so-net.ne.jp/kigiken/e_jp_steam.html
(extremely detailed data, albeit for a relatively small number of locomotive designs)
Steam Locomotive Design
Sinclair, Locomotive Engine: Running and Management (1890), online at
Barnes,”Gasoline Locomotives for Industrial Railways,” http://www.irsociety.co.uk/Archives/35/Gas_Locos.htm
[5AT] “The Engineering Design of the 5AT,”
“Steam Locomotive Designer,”
[Booty/WVG] Booty, “Steam Locomotive Walschaert Valve Gear Animation,”
[Booty/cbal] Booty, “Why are the Main Driver Counterbalances Not Symmetrical,”
Chapter 2: Railway Industry Overview
Horowitz, “THE VEHICLE –PROPULSION AND RESISTANCE”
(Davis formula for train resistance, takes air resistance into account)
Pitts, Principles of Locomotive Design
Thomas, Geared Steam Locomotive Works,
(comprehensive review of all of the geared locomotive designs)
Riedel, “Heisler Engine Design part I, Lower Engine,”
Luiz, “Gear reduction,” http://www.off-road.com/hummer/tech/gear.html
(good discussion of the effect of gear reduction on output torque)
Bourne, “A Catechism of the Steam Engine”
(Theoretical treatment of exhaust gas effect on draft)
http://www.spiraxsarco.com/esc/default.asp?redirect=WS_Properties.aspx (steam tables)
Loco Speed records:
Sites dealing quantitatively with subjects like loads on engine parts, and balancing the loads:
Rai University, Lesson 16, “Balancing of Rotating Masses,”
Lesson 17, “Balancing of Reciprocating Masses,” … -17.pdf;
Lesson 18, “Effect of Partial Balancing,” … -18.pdf;
Lesson 19, “Balancing of Forces in Engine,” … -19.pdf
Anon., “Engine Balance,” en.wikipedia.org/wiki/Engine_balance.html
Malm and Keast, “On-Line Compressor Rod Monitoring to Prevent Failures,” http://remtechnology.com/downloads/PDF%20Outputs/On-Line%20Compressor%20Rod%20Load.pdf
(pages 3-4, gas and inertial loads on piston rod)
Magnante, “Choosing the Right Connecting Rods,”
Lamar, “The Rotor Versus the Piston,”
Sacramento Sky Ranch, “Connecting Rod Balance in Continental and Lycoming Aircraft Engine,”
“Engine Excitation Mechanisms,” Science and Engineering Encyclopedia,
“How a locomotive is built” (1907)