US158525A - Improvement in air-vacuum engines - Google Patents

Improvement in air-vacuum engines Download PDF

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US158525A
US158525A US158525DA US158525A US 158525 A US158525 A US 158525A US 158525D A US158525D A US 158525DA US 158525 A US158525 A US 158525A
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air
pump
improvement
main cylinder
engines
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01BMACHINES OR ENGINES, IN GENERAL OR OF POSITIVE-DISPLACEMENT TYPE, e.g. STEAM ENGINES
    • F01B17/00Reciprocating-piston machines or engines characterised by use of uniflow principle
    • F01B17/02Engines

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  • Air-Vacuum Engine of which the following is a specication:
  • This engine is operated by a partial vacuum produced by cooling hot air. It has two cylinders, and transfers the air from one to the other, passing it through a cooler in transit. It receives the air hot and discharges it comparatively cold. As usually constructed, the engine receivesthe air at the pressure of the atmosphere and discharges it at the same pressure 5 but it may be made to work under an articial atmosphere of more than normal density, if preferred, by using tight covers on the two cylinders and exhausting into a receiver.
  • the engine in general construction, is composed essentially of a working'cylin der, acooler or condenser, and an airpump, with suitable valves and controlling means.
  • the inlet and outlet valves of the main cylinder are operated by cams or eccentrics; but the valves of the pump operate automatically by dii'erence of pressure, as usual.
  • the cooler or condenser O is arranged between the main cylinder A and the pump B. It is shown in the drawing as a double cylindrical vessel immersed in water, and having a cylindrical diaphragm in the interior to give greater length of current to the air being cooled. Other forms of condenser may be used, but not as well.
  • the cranks are arranged in such a manner that the pump upstroke begins before the piston of the main cylinder has completed its upstroke by about one-sixth of the stroke; The cranks are set about one hundred and thirty degrees apart.
  • the main cylinder A takes its supply of heated air direct from the furnace or other source of heat, and the inlet-valve of the main cylinder closes considerably before the completion of the upstroke, thus expanding the inclosed hot air in the main cylinder to any desirable point, and the expansion is subsequently carried still farther by the pump commencing to draw soon after the closure of the inlet-valve, which per mits the work of exhaustion in the pump to be performed, in a great measure, before any considerable portion of the air is cqoled.
  • rlhe stroke ofthe pump is, therefore, accomplished with much less power than would be required if the strokes of main piston. and pump were simultaneous and opposite each other; or, in other terms, the expansion of the heated air is carried out much farther with corresponding gain.
  • the character and amount of this gain are shown by diagrams on Sheet 2 of the drawings, marked l, 2, 3, and 4.
  • the power is derived from the unbalanced pressure of the atmosphere acting rst on the piston a of the main cylinder A, and afterward on the piston b ofthe pump B.
  • the inlet and outlet valves of the main cylinder are so operated by cams on the main shaft that one is closed before the other opens.
  • the inlet-valve should be open at the moment the main piston begins its upstroke, and may shut at any point in the stroke less than iive- ⁇ eighths of the whole stroke upward, according to the required degree of expansion.
  • the outlet-valve of main cylinder should open at the commencement of the upstroke of the pump.
  • the inlet-valve opens outward and the outlet inward.
  • the water being pumped is carried through the coolingchamber surrounding the condenser,'said cooling-chamber being simply a part of the suction or discharge pipe of the pump.
  • This en'- gine may take the hot air from the chimney of any ordinary iire or range, as when used for a household pumping-engine.
  • a special ire to operate the engine is dispensed with; or it may be run with gas-burners, arranged in a proper combustion-chamber; or it may have the air heated in a heater specially constructed, similar to that in my air-engine patented July 16, 1872; reissued March 25, 1873.
  • Sheet 2 represents diagrams as produced by the Well-known instrument termed the indicator.
  • Diagram 1 represents cards from the main cylinder A and from the pump B, superposed.
  • the cranks are arranged, as herein described, one hundred and thirty degrees apart.
  • the effective mean pressure in the cylinder, allowing nothing for leakage or friction, is six and one-half pounds per square inch.
  • Diagram 3 shows the theoretical cards superposed, Which would be taken from the main cylinder and pump if the cranks Were in the same plane, so that the main piston and the pump-piston rose and sank exactly simultaneously.
  • the effective mean pressure so arranged, allowing nothing for leakage or friction, would be only four and three-tenths pounds per square inch.

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  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Compressors, Vaccum Pumps And Other Relevant Systems (AREA)

Description

2 Seets--Sheet 2.
fA. K. mman. 'Air-Vacuum Engines.
`menm 1an. 5, 1375.`
Noxa-8,525'.
THE GRAPHIC CDAPHDTD-LITH3931 44 PARK PL^CE,N,Y.
UNITED STATES PATENT OEEIoEo ALEXANDER K. RIDER, OF VVALDEN, NEW YORK, ASSIGNOR TO RIDER, WOOSTER & OO., OF SAME PLACE.
IMPROVEMENT IN AIR-VACUUM ENGINES.
Specification forming part-of Letters Patent No.158,525, dated January 5, 1875; application tiled May 20, 1874.
To all whom it may concern:
Be it known that I, A. K. RIDER, of Walden, Orange county, in the State of New York, have invented an Improvement in Air-Engines, which may be termed an Air-Vacuum Engine, of which the following is a specication:
This engine is operated by a partial vacuum produced by cooling hot air. It has two cylinders, and transfers the air from one to the other, passing it through a cooler in transit. It receives the air hot and discharges it comparatively cold. As usually constructed, the engine receivesthe air at the pressure of the atmosphere and discharges it at the same pressure 5 but it may be made to work under an articial atmosphere of more than normal density, if preferred, by using tight covers on the two cylinders and exhausting into a receiver.
The engine, in general construction, is composed essentially of a working'cylin der, acooler or condenser, and an airpump, with suitable valves and controlling means. The inlet and outlet valves of the main cylinder are operated by cams or eccentrics; but the valves of the pump operate automatically by dii'erence of pressure, as usual.
The cooler or condenser O is arranged between the main cylinder A and the pump B. It is shown in the drawing as a double cylindrical vessel immersed in water, and having a cylindrical diaphragm in the interior to give greater length of current to the air being cooled. Other forms of condenser may be used, but not as well. The cranks are arranged in such a manner that the pump upstroke begins before the piston of the main cylinder has completed its upstroke by about one-sixth of the stroke; The cranks are set about one hundred and thirty degrees apart. The main cylinder A takes its supply of heated air direct from the furnace or other source of heat, and the inlet-valve of the main cylinder closes considerably before the completion of the upstroke, thus expanding the inclosed hot air in the main cylinder to any desirable point, and the expansion is subsequently carried still farther by the pump commencing to draw soon after the closure of the inlet-valve, which per mits the work of exhaustion in the pump to be performed, in a great measure, before any considerable portion of the air is cqoled. rlhe stroke ofthe pump is, therefore, accomplished with much less power than would be required if the strokes of main piston. and pump were simultaneous and opposite each other; or, in other terms, the expansion of the heated air is carried out much farther with corresponding gain. The character and amount of this gain are shown by diagrams on Sheet 2 of the drawings, marked l, 2, 3, and 4.
The power is derived from the unbalanced pressure of the atmosphere acting rst on the piston a of the main cylinder A, and afterward on the piston b ofthe pump B. The inlet and outlet valves of the main cylinder are so operated by cams on the main shaft that one is closed before the other opens. The inlet-valve should be open at the moment the main piston begins its upstroke, and may shut at any point in the stroke less than iive-` eighths of the whole stroke upward, according to the required degree of expansion. The outlet-valve of main cylinder should open at the commencement of the upstroke of the pump. The inlet-valve opens outward and the outlet inward.
In engines designed for pumping, the water being pumped is carried through the coolingchamber surrounding the condenser,'said cooling-chamber being simply a part of the suction or discharge pipe of the pump. This en'- gine may take the hot air from the chimney of any ordinary iire or range, as when used for a household pumping-engine. In that case a special ire to operate the engine is dispensed with; or it may be run with gas-burners, arranged in a proper combustion-chamber; or it may have the air heated in a heater specially constructed, similar to that in my air-engine patented July 16, 1872; reissued March 25, 1873.
Other constructions of cylinder and pump will serve, with some success, the purpose intended by this arrangement, provided that the main piston begins its upstroke before the former has completed its upstroke, whether it is by cross-connection or separate motion, or by beams or levers.
Sheet 2 represents diagrams as produced by the Well-known instrument termed the indicator. Diagram 1 represents cards from the main cylinder A and from the pump B, superposed. The cranks are arranged, as herein described, one hundred and thirty degrees apart. The effective mean pressure in the cylinder, allowing nothing for leakage or friction, is six and one-half pounds per square inch. Diagram 3 shows the theoretical cards superposed, Which would be taken from the main cylinder and pump if the cranks Were in the same plane, so that the main piston and the pump-piston rose and sank exactly simultaneously.
The effective mean pressure so arranged, allowing nothing for leakage or friction, would be only four and three-tenths pounds per square inch.
The exhaustive pump B, combined with the v
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