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ccumulators and dynamo-electric machines. [Illustration: NEW STEAMER PROPELLED BY HYDRAULIC REACTION.] We now arrive at Messrs. Maginot & Pinette's system, the description of which will be greatly facilitated by the diagram that accompanies this article. The inventors have employed a boat 14 meters in length by 1.8 m. in width, and 65 centimeters draught behind and 32 in front. The section of the midship beam is 70 square decimeters, and that of the exhaust port is 4. At a speed of 2.2 meters per second the tractive stress, K, is from 10 to 11 kilogrammes. At a speed of 13.5 kilometers per hour, or 3.75 meters per second, the engine develops a power of 12 horses. The piston is 19 centimeters in diameter, and has a stroke of 15 centimeters. The shaft, in common, of the pump and engine makes 410 revolutions per minute. It will be seen from the figure that suction occurs at the lower part of the hull, at A, and that the water is forced out at B, to impel the vessel forward. C and C' are the tubes for putting the vessel about, and DD' the tubes for causing her to run backward. Owing to the tubes, C, C', the rudder has but small dimensions and is only used for _directing_ the boat. The vessel may be turned about _in situ_ by opening one of the receiving tubes, according to the side toward which it is desired to turn. This boat is as yet only in an experimental state, and the first trials of her that have recently been made upon the Saone have shown the necessity of certain modifications that the inventors are now at work upon.--_La Nature_. * * * * * A NEW FORM OF FLEXIBLE BAND DYNAMOMETER. [Footnote: Read before Section G of British Association.] By Professor W.C. UNWIN. [Illustration: Fig. 1.] In the ordinary strap dynamometer a flexible band, sometimes carrying segments of wood blocks, is hung over a pulley rotated by the motor, the power of which is to be measured. If the pulley turns with left-handed rotation, the friction would carry the strap toward the left, unless the weight, Q, were greater than P. If the belt does not slip in either direction when the pulley rotates under it, then Q-P exactly measures the friction on the surface of the pulley; and V being the surface velocity of the pulley (Q-P)V, is exactly the work consumed by the dynamometer. But the work consumed in friction can be expressed in another way. Putting [theta] for the arc embraced by the be
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