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Mechanical Appliances and Novelties of Construction
by
Gardner D. Hiscox, M.E.
Norman W. Henley Publ. Co.
1927

The Inventor's Paradox - Desaguliers' Demonstration
The Prevailing Wheel Type
Marquis Of Worcester Wheel
Rolling Balls
Folding Arms
Chain Wheel
Most Common Idea
Magnetism And Gravity
Pick-up Ball
Ball-Carrying Belt
Ferguson's Type
French, 1858
Revolving Tubes And Balls
Geared Motive Power
Differential Hydrostatic Wheel
Lever Type
Double Cone
Rocking Beam
Titling Tray And Ball
Rolling Ring
Differential Water Wheel
Multiple Water Wheel
Gear Problem
Mercurial Wheel
Water Wheel
Air-Bag Wheel
Water Wheel
Air Transfer In Submerged Wheel
Extending Weights And Water Transfer
Chain Buckets
Congreve's Sponges
Transfer Of Air
Differential Weight of Balls
Inclined Disk And Balls
Self-Moving Water Power
Chain Pump, 1618
Archimedean Screw
Differential Weight By Flotation
Floatation Problem
Liquid Transfer Wheel
Chain-Pump
Mercurial Displacement
Air-Buoyed Wheel
Magnetic Resistance
Overbalanced Cylinder
Hydrostatic Weight
Capillary Attraction
Magnetic Pendulum
Magnetic Wheel
Magnetic Mill
Regenerating Pendulum
Magnetic Wheel
Alternate Magnet Type
Electro-magnetic Type
Electrical Generation
Perpetual-Motion Puzzle



23. Perpetual Motion
Congreve's sponges

     The sponge problem of Sir W. Congreve, of rocket fame. Three horizontal rollers are fixed in a frame; an endless band of sponge runs round these rollers, and carries on the outside an endless chain of weights surrounding the band of sponge and attached to it, so that they must move together, every part of this band and chain being so accurately uniform in weight that the perpendicular side will, in all positions of band and chain be in equilibrium with the hypotenuse, on the principle of the inclined plane.

Perpetual Motion Machine: 945-Congreve'sSponges

     The frame in which these rollers are fixed is placed in a cistern of water having its lower part immersed. On the perpendicular side of the triangle, the weights hanging perpendicularly alongside the band of sponge, the band is not compressed by them; and, its pores being left open, the water, at the point where the band meets its surface, will rise to a certain height above its level, and thereby create a load, which load will not exist on the ascending side, because on this side the chain of weights compresses the band at the water's edge, and squeezes out any water that may have previously accumulated in it, so that the band rises in a dry state, the weight of the chain having been so proportioned to the breadth and thickness of the band as to be sufficient to produce this effect.

(Subsection 945, from p.378)


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