Michael wrote:Haa... okay. Here goes Stewart, and everyone else who replied. believe me...it is good. If anyone makes this work... please, please remember me. And to John C. If this is imposing upon your idea, I apologize.
First of all the three things are the same thing. Think of a crab. As it moves side to side the legs on one side create an acute angle, and the legs on the other create an obtuse
angle. Look at the slider mech on the first and last drawing mentioned. It has the combination of the 2 different crab legs.
Now look at the last drawing. See the two weights attatched to the rods? Notice they are placed together? See the two circles the rods attatch to on the other end? Consider them to be two gear wheels of the same ratio. The interesting thig about this is, when the rods and weight are straight out horizontally, like in the picture, the leverage is balanced, and the weights don't move. If you were to tilt it clockwise, they still would not move because the upper weight (remember the term upper weight, as quoted by Bessler) has the greater leverage, and wants to move downwards, but because they are geared together it's pushing the lower weight up- and nothing can move because they are touching. But move it any slight angle counter clockwise, and the lower weight has greater leverage and it will swing down, and cause the upper to swing up, until they smack in to each other again on the other side, or until they stop by another means. Now think of the drawing that says "and still you do not understand?", and regard the angles. Consider the attatchement of this mech, by the gears to the rim of an inner cylinder "like a grindstone." and consider one pair, counter balanced by another on the other side, like in the last drawing. Now...Bessler said the greatest torque begins when the weights come to be placed together. Like in the drawing-out horizontally. This could be the driving force of the wheel. He also says the upper weight drives the force suppled to the "push" of the other parts? This could be the movement of the pairs, tilted on angle so as to cause them to seperate. Do you see what I mean? Part of their respective movements could also be by stationary angle, like shown in the main drawings, and as mentioned before by myself and Grim.
Thing is, there are so many variables of combinations with this idea. When Bessler said "the flail belongs to the farmer, not the scholar", he could have meant the solution will only come to the worker-the experimenter, because of the seemingly endless combinations of these mechs (if this is correct.) Like it came to him, possibly. And of course then John C, is correct in his advice.
I have a few other possible insites, I'll provide soon.
Best regards,
Michael
christo4_99 wrote:My idea of the construction is thus : The two thick black hoops are mounted to the axle by their own supports/bearings per so that they move freely and remain centered . The two round pendulums are fastened at their respective ends to the hoops at two places per , one per hoop . This causes the two round pendulums to move in duplicate . The two round pendulums have brass or other metal hollow spheres (the lowermost one slightly heavier than the other) along with a arm per fastened to their periphery and are movable within . The arms of the metal hollow spheres have chords attached to them so that they can be raised and lowered with tension and slack . The chords are attached as in the third illustration to a central arm which is attached to the outer hoop . The two round pendulums are arranged to contact the inner hoop as they move inward . The inner edges of the round pendulums are arranged to only contact the spokes of the wheel . The spheres are suspended in a liquid that may be capped with an appropriately shaped piece of wood or other object to prevent the fluid from moving chaotically . When the wheel is turned the pendulums are displaced thus causing the liquid within them to move and raising one sphere while lowering the other , this action gives slack to one sphere and as one sphere is lowered it pulls itself and the pendulum within which is is contained inward . As the liquid rocks back the other way from the spoke passing and another spoke displacing the higher pendulum the process reverses . In between the inward arms of the round pendulums there is a rod (weight ) which can rotate freely on the axle and is spun and returned both by a spring tension in the thin downward arms of the round pendulums and the ends of the round pendulums alternately . Note : when this rod is centered it is not affecting the machine for a brief instant and it's function is to convey the bulk of the pressure from the movement to the round pendulums alternately and to sustain the movement .