First law of Thermodynamics and energy conservation

Click For Summary

Discussion Overview

The discussion revolves around the First Law of Thermodynamics and the concept of energy conservation, exploring the implications of different types of systems (isolated, closed, and open) on energy changes. Participants seek to clarify how energy is conserved and transformed in various scenarios, including practical examples.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about the relationship between energy preservation and the equation ##\Delta{U}=Q+W##, questioning how energy can change if it is preserved.
  • Another participant clarifies that in an isolated system, both work ##W## and heat ##Q## are zero, leading to no change in internal energy ##\Delta U##, while in non-isolated systems, ##\Delta U## can change if ##W## and ##Q## are non-zero.
  • A participant distinguishes between open and closed systems, explaining that external forces affect open systems, while closed systems do not experience such forces. They provide an example involving a piston and gas to illustrate how work done on a system affects energy.
  • One participant attempts to categorize different systems, providing examples of open (boiling water without a lid), closed (pressure cooker), and isolated systems (thermoflask), while referencing a historical law of energy conservation.
  • Another participant acknowledges the helpfulness of previous explanations and reinforces the understanding of isolated systems where ##\Delta{U}=0=Q+W##.

Areas of Agreement / Disagreement

Participants demonstrate a mix of understanding and confusion regarding the First Law of Thermodynamics and the distinctions between system types. While some points are clarified, there remains uncertainty about the implications of energy conservation in different contexts, and no consensus is reached on the initial confusion expressed.

Contextual Notes

Participants discuss the definitions and implications of isolated, closed, and open systems, but there are limitations in their explanations, particularly regarding the nuances of energy transfer and transformation in various scenarios.

mcastillo356
Gold Member
Messages
660
Reaction score
365
Hi PF!
I don't understand the sentence: on one side says the energy is preserved, and, at the end, the total energy of the system will change if ##W## or ##Q## is added: ##\Delta{U}=Q+W##.
Greetings!
 
Science news on Phys.org
If a system is isolated, then ##W = Q = 0## and ##\Delta U = 0##, i.e. the energy of the system is constant. But if the system is not isolated, and ##W## and ##Q## are non-zero, then ##\Delta U## is not necessarily zero and the system energy not necessarily constant!
 
  • Like
  • Love
Likes   Reactions: vanhees71, Dale and mcastillo356
There is difference between a closed and an open system when law of conservation of energy is considered. If we have an open system, there are some resultant external forces acting on the system. If system is closed, there are no resultant external forces acting on the system.

Lets say we have a cylinder that is containing some volume V of the gas. The gas will be the (open) system in this example. If we push a piston, the volume V of the system will decrease. The piston had done work W on the system. By that, the energy of system (the gas) increased by exactly the amount of work that piston had done on the system.
If our (closed) system includes the gas, the piston and us, the total energy of the system will be the same before pushing the piston and after pushing the piston.

But, the total energy is the same in both cases: for open system the total energy is the energy of system + work done on the system. The work done on the system was not created from thin air. In example above we pushed the piston and for that we used some our internal energy.

I hope this helps. Sorry for bad English, I'm not native speaker :)
 
  • Like
  • Love
Likes   Reactions: mcastillo356 and vanhees71
Thank you very much, etotheipi, KMCv! Well, let's see if I understood: example of open system: me; boiling water without a lid. Closed system: a pressure cooker, just before the safety valve opens. Isolated system: a thermoflask (this is not true; it's slower, but it exchanges heat with its surroundings). In terms of energy, there is a law, first proposed and tested by Émile du Châtelet, witch states that energy cannot be created nor destroyed; only transferred or transformed.
KMCv, your post is very revealing: the difference between open and closed system is the same in thermodynamics and Newton's dynamics; and in your example of the cylinder containing gas, we can apply ##\Delta{U}=Q+W## the same if the system is open or closed.
ethoteipi, thank you very much for explaining the definition of isolated system: ##\Delta{U}=0=Q+W##. No work nor heat (neither mass) can pass to the system.
Greetings
 
  • Like
Likes   Reactions: KMCv
I'm happy that helped! :)
 

Similar threads

  • · Replies 46 ·
2
Replies
46
Views
6K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 37 ·
2
Replies
37
Views
5K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K
Replies
5
Views
851
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 1 ·
Replies
1
Views
1K