Friction make observing Newton's first law of motion difficult?

In summary, the conversation discusses the difficulty in observing Newton's first law of motion due to the presence of friction. The law states that an object will continue moving at a constant speed if no external forces act upon it. However, since there is always friction, an outside force is constantly acting on the object, making it difficult to observe the law. The conversation also touches on the definition of an inertial frame and how it relates to the first law, as well as the circularity of the definition and the role of Newton's second law in reasoning about external forces.
  • #1
WingZero
17
0
Why can friction make observing Newton's first law of motion difficult?
 
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  • #2
The friction would slow down the moving object, so if you didn't know it slowed down due to friction, then you could assume that there was no outside force slowing it down, so that kind of disproves the law.
 
  • #3
Newton's first law is kind of circular. We define the net absence of forces to be the state where an object moves uniformly.
 
  • #4
Another way to put that is: Newton's first law says that if there is no (outside) force, an object will continue moving at constant speed. Since there is always friction, there is NEVER "no outside force".
 
  • #5
Originally posted by Stingray
Newton's first law is kind of circular. We define the net absence of forces to be the state where an object moves uniformly.
Where did you find this definition? What is meant by "uniformly?"
 
  • #6
Originally posted by turin
Where did you find this definition? What is meant by "uniformly?"
i think he meant constantly or at rest.
 
  • #7
Yes, that's what I meant. Uniformly meant "without acceleration."

I didn't find the definition anywhere. It is my interpretation. Force is most naturally defined though Newton's 2nd law (generalization of the 1st law). What other definition would you like?
 
  • #8
Originally posted by Stingray
Yes, that's what I meant. Uniformly meant "without acceleration."

Force is most naturally defined though Newton's 2nd law (generalization of the 1st law). What other definition would you like?
Based on this, I can see why you think it is a circular definition. I myself had this problem not very long ago (I thought that the definition of "inertial frame" was circular, but I think it might be the same fundamental issue). The good news, at least for me, is that I got the conflict resolved, with the help of sereral contributors (of whom lethe was not the least).

Anyway, here's my resolution:

A rest frame is inertial if you can "connect" a mass to the origin by a massless spring, and the spring will not stretch.

It is a little figurative (not practicable), but the concept is sound, and it serves to eliminate the circularity, because the equilibrium point of the spring is well defined according to its rest length.

Now, Newton's first law says that free particles will move in straight lines with respect to such a frame (assuming space is flat).
 
  • #9
Originally posted by turin
Now, Newton's first law says that free particles will move in straight lines with respect to such a frame (assuming space is flat).

We seem to be thinking of different things. I didn't have an issue with the definition of an inertial frame. My internal picture was similar to what you described.

In your statement that I am quoting, I meant that labeling the particle as "free" is defined by its straight-line motion.
 
  • #10
Originally posted by Stingray
In your statement that I am quoting, I meant that labeling the particle as "free" is defined by its straight-line motion.
This is not true. A free particle is one that moves through a region of constant potential without constraint (since this is Newton's law, we're talking about mechanics in 17th century terms). This itself says nothing of the shape of the trajectory. That's where Newton's first law comes in. Given that there is no potential gradient and no surface onto which the particle is constrained, Newton says that the trajectory of such a particle is straight in an inertial frame and the velocity does not change.
 
  • #11
You can't define potentials without talking about how they affect trajectories.

Also, the title of this thread is a force that can't be described by a potential :smile:
 
  • #12
Originally posted by Stingray
You can't define potentials without talking about how they affect trajectories.
I'll have to think about this one. Just off the top of my head, I would say that you can, because energy is an abstraction that does not require a trajectory, so the same can be said of a potential, which is closely related to energy (energy/interaction factor). IMO, Newton's first law is how a potential affects a trajectory, and that the definition is just backwards, not circular.



Originally posted by Stingray
Also, the title of this thread is a force that can't be described by a potential :smile:
Yes, I agree. I think that would be a good reason why friction makes the first law difficult to observe.
 
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  • #13
Originally posted by Stingray
Newton's first law is kind of circular. We define the net absence of forces to be the state where an object moves uniformly.
I don't see how this is circular. What if we defined the net absence of forces to be when a body accelerates at 1 m/s2. Would that be circular? In any event, if Newton's first law were a definition, then we could write
No net forces act upon a body if and only if the body moves uniformly.
This is a defintion, so we must use the equivalence. In which case, I see no circular reasoning. However, Newton's first law says,
A body in will move in uniform motion unless acted upon by an external force.
which is equivalent to
If an external force does not act on a body, then the body will move in uniform motion.
which is not an equivalence.
If we then considered a body moving uniformly, and claimed that no external forces acted on the body, we would be using false logic. But the second law is not just a generalization of the first. The second law permits reasoning in the backward direction. It tells us,
A force F acting on a body gives it an acceleration a which is in the direction of the force and has magnitude inversely proportional to the mass m of the body.
Mathematically, a=F/m. This is an equivalence. So if we consider a particle with zero acceleration, we are permitted to conclude that no forces act on it.

Edit:
I should mention that we have defined acceleration to be a change in velocity. That is, a body does not move uniformly if and only if the body accelerates.
 
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  • #14
Originally posted by StephenPrivitera
if Newton's first law were a definition, then we could write
No net forces act upon a body if and only if the body moves uniformly.
Newton's first law is not a definition, is it?
 
  • #15
Originally posted by turin
Newton's first law is not a definition, is it?
No it is not, that was part of my point.
 
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1. How does friction affect an object's motion?

Friction is a force that opposes motion, so it can slow down or stop an object's motion. This can make it difficult to observe Newton's first law, which states that an object will continue to move at a constant velocity unless acted upon by a net external force.

2. Can friction cause an object to move without a force acting on it?

No, an object will not move without a force acting on it. Friction can only slow down or stop an object's motion, but it cannot initiate motion on its own.

3. How does surface type affect friction?

The type of surface an object is moving on can greatly affect the amount of friction present. Rougher surfaces typically have more friction, making it more difficult to observe Newton's first law of motion.

4. Is there a way to reduce or eliminate friction?

Yes, friction can be reduced or eliminated by using lubricants, such as oil or grease, between two surfaces. Additionally, using smoother surfaces or reducing the force between two surfaces can also reduce friction.

5. How do you calculate the force of friction?

The force of friction can be calculated using the formula F = μN, where F is the force of friction, μ is the coefficient of friction, and N is the normal force. The coefficient of friction depends on the surfaces in contact and the normal force is the perpendicular force exerted by one surface on the other.

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