Re: Understanding Mechanical Advantage by Brion To
Well, actually to me; the weight isn't transferred so much as the distance (if sitting in it on a pulley and starting pulling yourself up). For even at stand still; there is 1/2Load on each leg of support. So, a 100# climber would have 50# on each leg of line. When (s)he pulls down on the friction hitch side\ dynamic side; it just makes it 50# x 4'=200 ft pounds effort(for example)work, rather than perhaps just hanging by arm rather than friction hitch on that leg of line('costing' 50# effort). Which then becomes 2' out of each of the 2 legs=4', that raises the climber 2'.
i think a class or a sub class of the lever classes is missing, that is denoted by this (and other) scenarios. A 1st class lever is the only class that the input(effort, bodyWeight) and output(work on load) are separated by the pivot. So, this means that the input and output flow in opposite directions; another unique aspect of only the 1st class levers. Therein, comes this oft overlooked use/ class/ subclass to me. Because the 2 moving points are in opposite directions, this type of system can manipulate the equal and opposite forces that are promised in all things. So, because this comes from 2 points to 1 this recursive setup gives a compounding action.
A pulley by itself is a 1stClass Lever, but the systems are broke into the 3 pulley classes by the position of that 1stClass Lever, the pulley. Of the 3 positions (inputEffort, pivot/anchor, outputWork on load); if the pulley is on the input we increase speed/ lose power like in a 3rd class lever (where the input is closer to the anchor/pivot) with input and outputs moving in the same direction. If we place pulley on the pivot/anchor position, we have a neutral 1st class lever, with input and outputs moving in opposite directions. And if the pulley is on the load, we have a 2nd class lever(with input further from pivot/anchor than load), with input and outputs moving in the same direction.
But, if we are hanging as ballast to a load, with pulley on overhead anchor/ 1st class position, and pull up on the rope going to load, we get our weight + 2xEffort on the lift/ballast on the load. With a foot cam, we can get 2xLegForce + bodyWeight, rather than 2xArmForce + bodyWeight.
Now, that has to be 1st class to move input of bodyWeight and passiveForce from effort of hand on other line moves down as it lifts up on load, but then can't be 1st class, because that effort hand on the load side is headed the same direction as the load.... The same can be configured on non-rolling levers (wood, metal etc.), to get 1xWeight + 2xEffort, but needs pivot between. Stand on one side of see saw, load just over pivot on other side, your bodyWeight pushes load up, and if you go to pick load up with 50# effort, you 'lighten' 50# off the load side of the seesaw, while 'increasing your bodyWeight' that is pushing up on the 50#(+ bodyWeight) lighter load by 50#... So your 50# effort gives 100# lift upwards as long as load is still on see saw. Once again with 1 pivot, we are moving inputs both with and against the direction of the load....
i've never been sure of de-scribing pulley systems in leverage class terms anyway. For, pulleys operate in 1 dimension only, as they are inline, not 'leveraged angle' devices. Now, bending across a tight line is leveraging to me, just like forcing across the long axis of a lever. A pulley's system increases leverage by adding another leg. But if we give a stool a 4th leg, do we say we have increased it's leverage?? we would only say that the leg is leveraged on the stool.. if the leg was at an angle, and thereby something changed direction as it progressed any movemeant. But, the example of a double use of force by capturing it's promised equal and opposite force and folding it back to work on the load exists in the non-flexible levers too.