US9127A - Fibe-eetgote - Google Patents

Fibe-eetgote Download PDF

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Publication number
US9127A
US9127A US9127DA US9127A US 9127 A US9127 A US 9127A US 9127D A US9127D A US 9127DA US 9127 A US9127 A US 9127A
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United States
Prior art keywords
lever
arm
stroke
axis
levers
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Expired - Lifetime
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F04POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
    • F04BPOSITIVE-DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS
    • F04B47/00Pumps or pumping installations specially adapted for raising fluids from great depths, e.g. well pumps
    • F04B47/02Pumps or pumping installations specially adapted for raising fluids from great depths, e.g. well pumps the driving mechanisms being situated at ground level
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10TTECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
    • Y10T74/00Machine element or mechanism
    • Y10T74/18Mechanical movements
    • Y10T74/18888Reciprocating to or from oscillating
    • Y10T74/1892Lever and slide
    • Y10T74/18928Straight line motions

Definitions

  • Figure l is a perspective view of a tire engine to which my improved combination of levers is applied;
  • Fig. 2 is a side elevation of the levers detached;
  • Fig. 3 is a plan of the same;
  • A is the body of theengine supported by a carriage as represented and containing the pumps and their appendages; B, B is a frame to support the axes of the levers and C, C are arms by which they are worked; D is one of the pump cylinders and E the air chamber all which parts may be constructed and arranged in the usual manner or otherwise; a, a is a double lever strengthened by the side braces f, f and vibrating on the axis l which rests in suitable bearings in the frame B, B; o, is a short lever with equal arms vibrating on the axis e which rests in bearings so placed that it may be parallel to the axis d; each arm of the short lever is divided vertically by a space sutilcient to allow 'an arm of the long lever to work freely between the two divisions7 and at the end of the arm a friction roller c extends across these two divisions or from one to the other upon which the arm of the long lever rests.
  • the axis e is placed above the axis (Z as represented in the drawing and both levers have a bent or curved form s0 that each arm of the long lever a, a may pass between the two divisions of an arm of the short lever I) and act against the friction roller c.
  • the pump rod h is connected to the short lever I) and is hung in a cavity inthe piston (within the cylinder D) by a pin passing through it so as to allow it to vibrate and accommodate itself to the curvilinear motion of the point of connection on the lever b, b.

Description

' UNITE STATES ATE irme
ORVILLE G. ADKINS, OF OSVEGO, YEVVv YORK.
FIRE-ENGINE.
To all whom it may concern Be it known that I, ORVILLE G. ADKINs, of Oswego, in the county of Oswego and State of New York, have invented a new and Improved Combination ot Levers for IWorking Fire-Engines and for other `Purposes; and I do hereby declare that the same is described and represented in the following speciiication and accompanying drawings.
It is well known that the common fire engines, as well as most of the different species of forcing pumps have an air chamber attached to them and that the force of the stroke is directly applied to the compression of the air therein confined, its elastic reaction raising o-r forcing out the water; and as the elastic force of compressed air is exactly proportionate to the amountof compression, or, in other words7 inversely proportionate to the space it occupies it is evident that for each stroke of the piston the resistance to be overcome is continually increasing from the beginning to the end of it. On the other hand in the case of the fire engine when the moving power is commonly the strength of man (and also in some other cases) the position of the lever arms toward the end of the stroke is much less favorable for the application of the power and consequently the eiiiciency of the force or power in operation may be said to be con tinually diminishing from the beginning to the end of the stroke. It is, doubtless, to this inverse ratio between the resistance and the efficiency of the power by which it is to be overcome, that the well known wear ing and exhausting effectot' working a fire engine is in great measure due; the vigor of the stroke being wasted before the strongest resistance is met a. severe and eX- hausting eiiiort is required to overcome that resistance and complete the stroke. To remedy this inconvenience and serious evil I have invented a combination of levers so connected and arranged that as the stroke progresses the relation between the lengths of the long and short arms of the main lever is continually changing by the motion of the point at which the resistance is met, the long arm or that to which the power is applied becoming longer and the short arm shorter: thus speed is given to the first part of the stroke and to the latter part the etlicient force required.
To enable others skilled in the art to make and use my invention I will proceed to describe its construction and operation referring to the drawings above mentioned in which the same letters indicate like parts in all the figures.
Figure l is a perspective view of a tire engine to which my improved combination of levers is applied; Fig. 2 is a side elevation of the levers detached; Fig. 3 is a plan of the same;
A, A is the body of theengine supported by a carriage as represented and containing the pumps and their appendages; B, B is a frame to support the axes of the levers and C, C are arms by which they are worked; D is one of the pump cylinders and E the air chamber all which parts may be constructed and arranged in the usual manner or otherwise; a, a is a double lever strengthened by the side braces f, f and vibrating on the axis l which rests in suitable bearings in the frame B, B; o, is a short lever with equal arms vibrating on the axis e which rests in bearings so placed that it may be parallel to the axis d; each arm of the short lever is divided vertically by a space sutilcient to allow 'an arm of the long lever to work freely between the two divisions7 and at the end of the arm a friction roller c extends across these two divisions or from one to the other upon which the arm of the long lever rests. The axis e is placed above the axis (Z as represented in the drawing and both levers have a bent or curved form s0 that each arm of the long lever a, a may pass between the two divisions of an arm of the short lever I) and act against the friction roller c. The pump rod h is connected to the short lever I) and is hung in a cavity inthe piston (within the cylinder D) by a pin passing through it so as to allow it to vibrate and accommodate itself to the curvilinear motion of the point of connection on the lever b, b. Now as the axis e is placed above the axis l it is evident that as an arm of the lever a, a descends the roller c must move along that arm toward the fulcrum or the axis d; thus the long arm of the descending half of the double lever a, a is becoming longer and the short arm (from c to d) shorter during the descent and consequently the force with which it acts is continually becoming greater in proportion to the power by which it is acted upon during the whole descent of the arm or from the beginning to the end of the stroke while according to a well known principle of mechanics the motion of the point of resistance or of the arm of the lever I), b is at -the same time and at precisely the same rate becoming less rapid inaproportion to that of the moving power. The important advantages arising from these results have been already pointed out. During the ascent the motion of the roller c or of the point of resistance along the lever a, a is of course the reverse of what has been just described and it will be seen that if the levers are so adjusted as to'bring the long lever in Contact. with both rollers when it has a horizontal position as in Fig. 2 and it is designed that it shall remain in contact with both, the curves on the lever a, a, on the opposite sides of each roller, must be similar curves; and that by varying the distance between the aXes e and Z and the form of the curves on the lever a, a the extent of the motion of the roller c along a, a and its rate at different points and consequently the extent and rate at vlong arm and shortening the short arm of the lever substantially as described.
In testimony whereof, I have hereunto signed my name before two subscribing witnesses.
ORVILLE G. ADKINS. l/Vitnesses A. F. ALLEN, O. C. BLOFE.
US9127D Fibe-eetgote Expired - Lifetime US9127A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2587627A (en) * 1944-12-26 1952-03-04 Lovell Mfg Co Wringer

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2587627A (en) * 1944-12-26 1952-03-04 Lovell Mfg Co Wringer

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