Is Work Directly Related to Time in Physics?

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Discussion Overview

The discussion centers on the relationship between work and time in physics, exploring whether work is explicitly dependent on time or if time plays an implicit role in the concept of work. Participants examine definitions, examples, and the implications of force and distance in the context of work, power, and energy transfer.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the definition of work is not related to time, emphasizing that work is defined as W=Fs, where F is the force and s is the distance.
  • Others argue that while work is not explicitly defined via time, the concept of time is inherently involved when considering how forces act over distances.
  • One participant points out that the net force can be considered in different contexts, suggesting that it can be the net force or any applied force, which complicates the discussion.
  • Several examples are discussed, including the scenario of a car decelerating, where participants explore how acceleration and distance relate to work done, questioning whether time influences these relationships.
  • There is a contention regarding whether the work done is the same in different scenarios, with some insisting that the total work remains constant regardless of the time taken to perform it.
  • One participant expresses confusion about the proportionality of acceleration and distance, seeking clarification on the relationship between these quantities in the context of work.

Areas of Agreement / Disagreement

Participants generally disagree on the role of time in the definition and understanding of work. While some maintain that work is independent of time, others suggest that time implicitly affects the dynamics of how work is done. The discussion remains unresolved with competing views on the relationship between work, force, distance, and time.

Contextual Notes

Participants reference specific examples and definitions from physics literature, indicating that interpretations may depend on context and specific scenarios. The discussion highlights the complexity of relating work to time, particularly in cases involving variable forces and acceleration.

gentsagree
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I just read that the definition of work is not related whatsoever to the notion of time, whereas the relation between time and work is expressed by the explicit notion of power. However, W=Fs, and F is proportional to the acceleration a, which is the change of rate of the velocity wrt time.

Could you clarify this? Is the solution merely that the work W is not EXPLICITLY dependent on time?
 
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gentsagree said:
However, W=Fs, and F is proportional to the acceleration a,
F is not the net force, but any force applied to an object.

gentsagree said:
Is the solution merely that the work W is not EXPLICITLY dependent on time?
It is nor defined via time. But of course you can compute the time for some energy transfer, given some extra information.
 
I don't agree with your first reply: F can be taken as the net force [check page 186 of Young and Freedman, for one].

Regarding the second point: I know it is not defined via time, I am just pointing out (naively, I know, but I'd like a better understanding) that implicitly in the notion of work we have that of time. Not only that, it is changing time, so something like Delta t.
 
gentsagree said:
F can be taken as the net force
It can, but it's not in general. You can't make general statements based on special cases.
 
gentsagree said:
I don't agree with your first reply: F can be taken as the net force [check page 186 of Young and Freedman, for one].
You're both right (or more accurately, correctly describing subtly different things).

The total amount of kinetic energy imparted when moving an object is the net force times times the distance. In many problems that's the useful work done and the only thing we care about.

However, if the net force is the sum of multiple opposing forces, the total amount of work done may be much greater. For example, if you are pushing an object at constant speed against the force of friction, the net force is zero and the kinetic energy of the object doesn't change; but you're clearly doing work and the energy ends up as waste heat.

I am just pointing out (naively, I know, but I'd like a better understanding) that implicitly in the notion of work we have that of time. Not only that, it is changing time, so something like Delta t.
I don't see this. Apply a force of 100N over a distance of 100 meters and you've done 10,000 Joules of work. It doesn't matter whether it took a millisecond or a century to cover that distance, the work done is the same.
 
Nugatory said:
I don't see this. Apply a force of 100N over a distance of 100 meters and you've done 10,000 Joules of work. It doesn't matter whether it took a millisecond or a century to cover that distance, the work done is the same.

I was thinking of this example: the velocity of a car which hits a wall goes from, say, 80 to 0 km/h almost instantaneously (quite disastrously). The force applied is then F=ma, where the acceleration is great since it happened over the space of a very short time interval. The work the brakes did is then W=Fs.

If the car gradually decelerates from 80 to 0, in say 10 seconds, the acceleration is much smaller. Hence the force and the work exerted by the brakes decrease.

This is why I was thinking that, implicitly, the work depends on time. Am I wrong?On a different note, please disregard my original comment on power: that's a completely different thing, just being the obvious description of how work is spread over time, thus a different aspect of time of what I wonder about.
 
gentsagree said:
I was thinking of this example: the velocity of a car which hits a wall goes from, say, 80 to 0 km/h almost instantaneously (quite disastrously). The force applied is then F=ma, where the acceleration is great since it happened over the space of a very short time interval. The work the brakes did is then W=Fs.

If the car gradually decelerates from 80 to 0, in say 10 seconds, the acceleration is much smaller. Hence the force and the work exerted by the brakes decrease.

This is why I was thinking that, implicitly, the work depends on time. Am I wrong?
Yes, you are wrong. The net work done in both cases is the same and is independent of the time it takes for the car to be brought to rest. (In the second case, while the force is reduced the distance increases.)
 
gentsagree said:
This is why I was thinking that, implicitly, the work depends on time. Am I wrong?
You can construct some scenario where some quantity depends on some other quantity. All physical quantities can be related somehow.
 
I think you've misunderstood something somewhere along the line so:

Work = Force * Distance

for a constant force. For a variable force you use an integral.

In your example involving the car, the car has high Force and low Distance when it hits the wall. It has low Force and high Distance when it slows down over a longer distance. The work for the two operations must be equal.
 
  • #10
That's right. Thank you.
 
  • #11
For some weird reason I was convinced that the increase in acceleration and the decrease in distance weren't exactly proportional. All sorted then. Merci
 
  • #12
They are exactly proportional. You can try constructing a few scenarios of your own and working them out mathematically if you're not convinced. Have a nice day!
 

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