- Joined
- Apr 16, 2010
- Messages
- 660
- Reaction score
- 3
#1 - I'm not sure if some of you read the lecture by EK regarding work done by Friction in EK, but it just totally confused my understanding of work. Based on what I read elsewhere (TPR & TBR), they mentioned nothing about needing to know the increase in internal energy of an object experiencing a frictional force over a distance, but apparently EK says it's necessary to find the work done by friction.
Work by Friction = Change in Energy of System
Fk x distance = delta PE + delta KE (lost) + delta Internal Energy (gained)
On the other hand, TPR and TBR instead just assume that the total change in mechanical energy is enough to find the amount of work done by friction.
Which is right?
#2 - Then they go on to mention that it's necessary to consider heat changes on your system. A lot of Physics equations for Work are based on the assumption that there's no heat changes involved. If there is a heat change, how does that factor in? Do we just subtract is from the total change in energy (since delta E = q + W)
#3 - Another confusion is work done by conservative forces: When do I assume that the total work is 0 J?
Can anyone help clarify this whole topic, I'm so confused lol.
Work by Friction = Change in Energy of System
Fk x distance = delta PE + delta KE (lost) + delta Internal Energy (gained)
On the other hand, TPR and TBR instead just assume that the total change in mechanical energy is enough to find the amount of work done by friction.
Which is right?
#2 - Then they go on to mention that it's necessary to consider heat changes on your system. A lot of Physics equations for Work are based on the assumption that there's no heat changes involved. If there is a heat change, how does that factor in? Do we just subtract is from the total change in energy (since delta E = q + W)
#3 - Another confusion is work done by conservative forces: When do I assume that the total work is 0 J?
Can anyone help clarify this whole topic, I'm so confused lol.