Feynman's reversible lifting machine analogy- help

In summary, the author is trying to explain the impossibility of building a machine that will lift a weight higher than it will be lifted by a reversible machine. He uses an example of two machines, one which lifts a weight a distance and the other which lowers a weight a distance. He proves that it is impossible to build a machine that will lift a weight higher than it will be lifted by the reversible machine.
  • #1
christian0710
409
9
Hi I'm having a very hard time trying to picture an argument in Feynmans physics volume one ). I can't picture this example he is talking about, so I wrote it down from the book and really hope someone can help me answer the question in the bottom.

From the book (everything needed to know is included)

Call this
reversible machine, Machine A. Suppose this particular reversible machine lifts
the three-unit weight a distance X. Then suppose we have another machine, Machine
B, which is not necessarily reversible, which also lowers a unit weight a
unit distance, but which lifts three units a distance Y. We can now prove that Y
is not higher than X; that is, it is impossible to build a machine that will lift a
weight any higher than it will be lifted by a reversible machine.
Let us see why.
Let us suppose that Y were higher than X. We take a one-unit weight and lower
it one unit height with Machine B, and that lifts the three-unit weight up a distance
V. Then we could lower the weight from Y to X, obtaining free power, and use
the reversible Machine A, running backwards, to lower the three-unit weight a
distance X and lift the one-unit weight by one unit height. This will put the
one-unit weight back where it was before, and leave both machines ready to be
used again! We would therefore have perpetual motion if Y were higher than X,
which we assumed was impossible. With those assumptions, we thus deduce that
Y is not higher than X, so that of all machines that can be designed, the reversible
machine is the best.


I don't get this part:
We can now prove that Y
is not higher than X; that is, it is impossible to build a machine that will lift a
weight any higher than it will be lifted by a reversible machine.


Why can't Y (the distance lifted by machine A) be highter than X (distance lifted by machine B)?? I assume both machines have same proportions (are able to reach the same maximum height) and both machines lift 3 units of weight a distance by lowering one unit a distance. So what physical law says that Machine B lift 3 units as high as machine A?
 
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  • #2
And what kind of a picture am I to Imagine in this sentence
"We take a one-unit weight and lower
it one unit height with Machine B, and that lifts the three-unit weight up a distance
V."
Is it that we lower the one unit weight of machine A with machine B, or do we just lower the weight of machine B one unit?
 
  • #3
I have tried to draw and illustrate my interpretation of A and then
drawn machine B according to this sentence

We take a one-unit weight and lower
it one unit height with Machine B, and that lifts the three-unit weight up a distance
V.


[PLAIN]http://i50.photobucket.com/albums/f317/christian0710/Computer/distanceup_zpsf7b187cc.jpg[/PLAIN]

But what happens after we have lifted the 3 units of machine B the height of v?
This is the sentence I can't visualize

Then we could lower the weight from Y to X, obtaining free power, and use
the reversible Machine A, running backwards, to lower the three-unit weight a
distance X and lift the one-unit weight by one unit height.
 
  • #4
I don't get this part:
We can now prove that Y
is not higher than X; that is, it is impossible to build a machine that will lift a
weight any higher than it will be lifted by a reversible machine.
Basicaly he is saying a balance of the weights is the most efficient that can be acheived.Or the weights can at best arrive at a position where they are balanced and no more.Otherwise it would be possible to build a perpetual motion machine if you could lift a weight higher in the reverse or other direction when the same force is applied.
 
  • #5
The clue to understand

If you read carefully the statement , you see the term "lower" is written in slight italics , which has deeper meaning in it, let's see what.

1. Reversible machine : can be restored without any external work done on it.

2. Irreversible machine : need some work to lift it to restore it . That is someone has to do work on the system to make it work again.

3. Perpetual machine : This machine lifts more than the reversible machine that means , to restore it
you have to lower it ,implies there is some power left in the machine , because when you lower it from Y to X the other side get lifted too to some height which is less than a foot (say this height k from ground). and therefore the machine can lift something else, for instance to restore the reversible machine.


Another way to think this Perpetual machine (Machine B) , and why they can't exist .
suppose i have a perpetual machine which contrary to reversible machine(machine A) lifts it to a greater height ,alright let's bring it down we now have some free work which can be used , but we will use it to the machine itself , Now let's say Y-X=C which is the difference in height it lifts ,which implies when we restore and again drop it down to the ground. Now clearly this device is going to lift the same higher than c (say c>>) , then in next step we make it down and lift again , this time the lifting goes c>>> , and so on it goes higher and higher.

The conclusion is that each time the machine lifts C units higher , now this can only happen that each time some external agency is working , and iff the machine is self sustaining then it has to be a perpetual machine.

Next post , I shall post the mathematical translation of it .

thanks
 
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Likes tarun purohit

What is Feynman's reversible lifting machine analogy?

Feynman's reversible lifting machine analogy is a thought experiment proposed by physicist Richard Feynman to illustrate the concept of thermodynamic reversibility. It involves a machine that lifts a weight using a reversible process, meaning that the process can be reversed with no energy loss.

Why is this analogy important in thermodynamics?

This analogy is important in thermodynamics because it helps us understand the concept of energy conservation and reversibility in thermodynamic processes. It also highlights the difference between ideal and real-world processes, as real-world processes are often irreversible and result in energy loss.

How does the analogy explain the second law of thermodynamics?

Feynman's analogy illustrates the second law of thermodynamics, which states that in any natural process, the total entropy of a closed system always increases. In the analogy, the lifting machine represents a closed system, and the lifting and lowering of the weight represents the increase and decrease of entropy, respectively.

What are the limitations of this analogy?

One limitation of this analogy is that it simplifies the concept of thermodynamic reversibility and does not take into account the effects of friction, which can result in energy loss even in a reversible process. It also does not consider the role of time in thermodynamics, as real-world processes take place over a finite period of time.

How can this analogy be applied in real-world situations?

This analogy can be applied in real-world situations by helping engineers and scientists design more efficient and reversible processes. It can also be used to understand and analyze the limitations and trade-offs of different thermodynamic systems and processes.

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