NET Force on Massless Body: Acceleration & Spring Force

In summary, when the net force on a massless body is 0, the acceleration can be anything. This is because, according to Newton's 2nd Law, F=ma, and when mass is 0, the force is also 0. The concept of a massless object is not applicable in classical physics as it leads to paradoxes, but in relativity it is possible. Similarly, if a massless spring is pulled with unequal forces on either side, the net force is 0 and the spring force is equal in magnitude and opposite in direction. This concept does not apply to gravity, magnetism, or other forces that do not require interaction with mass.
  • #1
atavistic
106
0
What happens when the NET force on a massless body is 0. I mean what will be the acceleration , if any?

Also if we pull a massless spring, from one side with a force F1 and from the other side a force F2, what will be the spring force?
 
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  • #2
I suppose some neutrinos are supposed to be massless and acceleration could occur if the neutrino interacted with an atom (converting neutrino energy to kinetic energy).
Also if we pull a massless spring, from one side with a force F1 and from the other side a force F2, what will be the spring force?

If F1 and F2 are constant, but unequal, the massless spring would likely instantly reach the speed of light.
 
  • #3
atavistic said:
What happens when the NET force on a massless body is 0. I mean what will be the acceleration , if any?

Like anything else, it will obey Newton's 2nd Law:

F = m a
or
0 = 0 x a

So, the acceleration can really be anything.

Also if we pull a massless spring, from one side with a force F1 and from the other side a force F2, what will be the spring force?

The net force must be zero for a massless object:

F = m a = 0 x a = 0

Therefore, F1 and F2 are equal in magnitude and act in opposite directions. Use either F1 or F2 in the spring formula,
F = k x
 
  • #4
Hi Redbelly,

F = m a
or
0 = 0 x a


So, the acceleration can really be anything.
In practice, acceleration is limited by the speed of light. For example: the speed of light limits quantized acceleration of a neutrino.

The net force must be zero for a massless object:

F = m a = 0 x a = 0
The original problem did not specify that F1 and F2 are equal or that the force is gravitational. Magnetism, the electrostatic field of a point charge and many other forces do not require interaction with mass. In other words, net F does not necessarily equal zero.
 
  • #5
pzlded said:
Hi Redbelly,
The original problem did not specify that F1 and F2 are equal or that the force is gravitational. Magnetism, the electrostatic field of a point charge and many other forces do not require interaction with mass. In other words, net F does not necessarily equal zero.

The original problem specified a massless spring. Therefore net force is zero, and F1 and F2 are equal in magnitude.

I don't see why you're bringing up gravity, magnetism, etc. These are beginning "Physics 101" concepts at play here.

Regards,

Mark
 
  • #6
Hi Mark,

Also if we pull a massless spring, from one side with a force F1 and from the other side a force F2, what will be the spring force?

The forces pulling on the spring could have been the result of a mass suspended by the spring. Perhaps I should have mentioned that if F1 equals –F2, the weight of the mass equals the pull on that end of the spring, equals the pull on the supporting bracket.

When F1 does not equal -F2, the spring could result in accelerate to light speed. However, this requires that the assembly of forces and a spring are massless and isolated.

Best Wishes
 
  • #7
redbelly, I am talking about the case when a spring is kept on a horizontal surface, and if a pull of magnitude F1 and F2 (not equal) respectively are given to the ends. Then how will F1 = -F2. For e.g. I give a force of 10 N and 20N , then for the spring

10 - 20 = m *a
=> 10 =0 !?

pzlded: Is there any proof for your claim?
 
  • #8
This is exactly why, in classical physics, there's no such thing as zero mass (I once asked a similar question about zero resistance in an introductory EE class... the answer is about the same).

The answer is, you "can't" apply a net force to a zero mass. It's just against the rules. If you do, you have a paradox, which just means that your description of reality was wrong... and it was! There are no classical massless objects, which is the only reason all values of force applied on any object are OK.

So the answer is throw away that "zero mass"; it's nonsense for precisely the reason you show. In relativity, however, zero mass is just fine, and it can experience forces, but that's only because the laws of physics get changed around so F doesn't equal m a anymore.
 
  • #9
If there is zero force on a zero mass, then RedBelly is correct: the acceleration can be whatever you like. It is "unconstrained" as a technical person would say. Of course this is kind of silly, but that's only because zero mass is silly to begin with.
 
  • #10
atavistic said:
What happens when the NET force on a massless body is 0. I mean what will be the acceleration , if any?
When you use the term "mass" do you mean rest mass or inertial mass? If you mean inertial mass then the acceleration can be anything you'd like. If the mass is zero then that means that the momentum is zero regarless of the velocity. Since force is the time rate of change of momentum it follows that the force is zero so this is consitent with the condition of zero force you are imposing.
Also if we pull a massless spring, from one side with a force F1 and from the other side a force F2, what will be the spring force?
What is this spring force that you speak of?

Pete
 
  • #11
Xezlec said:
If there is zero force on a zero mass, then RedBelly is correct: the acceleration can be whatever you like. It is "unconstrained" as a technical person would say. Of course this is kind of silly, but that's only because zero mass is silly to begin with.
What's so silly about zero mass?

It theoretically possible within the theory of relativity, although perhaps not in practice. Even negative values of mass have been discussed in the physics literature. Stress contributes to the inertial mass of a body while tension subtracts from it. I.e. there could be enough tension in a body to reduce its inertial mass to zero.

Pete
 
  • #12
pmb_phy said:
What's so silly about zero mass?

It theoretically possible within the theory of relativity, although perhaps not in practice. Even negative values of mass have been discussed in the physics literature. Stress contributes to the inertial mass of a body while tension subtracts from it. I.e. there could be enough tension in a body to reduce its inertial mass to zero.

Pete

As has been pointed out, this is the classical physics forum and it's a classical physics question. I mentioned parenthetically in my first reply that zero mass was perfectly fine in relativity.
 
  • #13
Xezlec said:
So the answer is throw away that "zero mass"; it's nonsense for precisely the reason you show.
It's nonsense in first question.

The second question is nonsense also, but not because the spring is massless. Massless springs are an idealization meant to get rid of complexities. An ideal spring is massless, frictionless, unbreakable, and has a force response that is a proportional to displacement (regardless of the frequency of the dispacement). A single massless spring often has one end fixed to a wall. Think of the wall as an object with infinite mass. The fixed end of the spring isn't going anywhere, so you don't even have to model the force at that fixed end. Massless springs are also modeled as having massive objects attached at each end. A bit tougher, but the ensemble is not massless.

Bottom line: A free-moving massless body makes no sense in classical physics. Don't ask questions about them because such questions are nonsense. A massless spring always has one end fixed to a massive object. The spring is not going to fly off at infinite speed. Don't ask questions about massless springs without any attached masses because such questions are nonsense.
 
  • #14
Hi D.H.

I rebel at the thought that physics is cut and dry. I do not object to the idea that classical physics is an idealization of the real world; I object to the idea that the difference between classical physics, quantum physics and relativity are almost by definition ‘unexplainable’. Together, these disciplines are contemporary and relevant to today’s workplace problems.

The lack of explanation of differences between classical physics and other physics can cause arbitrary declarations. Consider atomic collision products that travel that travel at light speed. Perhaps all those products must have no mass, perhaps they have ‘inherent’ mass, or maybe they have more mass than either the original target mass or projectile mass alone.

Best wishes
 
  • #15
pzlded said:
I rebel at the thought that physics is cut and dry.
Rebel all you want. Physics is supposed to be cut and dry because it is science. If you want the answer to be whatever you want, study philosophy or shudder postmodernism. Physics needs to be cut and dry so that we can make predictions, falsify hypotheses, and develop really neat and useful things such as the science behind the computer on which I am typing this post.

I do not object to the idea that classical physics is an idealization of the real world; I object to the idea that the difference between classical physics, quantum physics and relativity are almost by definition ‘unexplainable’.
Scare quotes. Please go back to your postmodernism studies. But please do bone up on physics while you go.

The difference between classical physics and quantum mechanics is anything but `unexplainable'. We know quite well what the differences are, where they lie, and how they come about. The same is true for classical physics and relativity. The same is not true for quantum mechanics and relativity. Physicists don't like that, so some are working on rectifying the situation.

Together, these disciplines are contemporary and relevant to today’s workplace problems.
Pretty please, go back to your postmodernism studies!

The lack of explanation of differences between classical physics and other physics can cause arbitrary declarations.
Pretty please, with sugar on it?

Consider atomic collision products that travel that travel at light speed. Perhaps all those products must have no mass, perhaps they have ‘inherent’ mass, or maybe they have more mass than either the original target mass or projectile mass alone.
Atomic collision products that travel at light speed have a name: photons. Photons have zero rest mass and a non-zero momentum given by [itex]E=hf[/itex]. Pretty cut and dry if you ask me.
 
  • #16
Perhaps all those products must have no mass, perhaps they have ‘inherent’ mass, or maybe they have more mass than either the original target mass or projectile mass alone.

The results of experiment disagree. If you're going to make this bizarre claim, you'd better have some really good evidence. Things that go the speed of light are massless. There's no mystery about this to people who have studied the subject via experiment.

Quantum physics is a more accurate approximation than classical physics. That's why it replaced it.
 
  • #17
atavistic said:
redbelly, I am talking about the case when a spring is kept on a horizontal surface, and if a pull of magnitude F1 and F2 (not equal) respectively are given to the ends. Then how will F1 = -F2. For e.g. I give a force of 10 N and 20N , then for the spring

10 - 20 = m *a
=> 10 =0 !?

Xezlec answered it well in post #'s 8 and 9. I'll just add:

Since zero-mass mechanical springs don't really exist, instead imagine that the spring's mass is much much less than ordinary everyday massive objects that are normally attached to that spring. For example, a spring might be 0.1 kg, and be connected to 100 kg objects. That's a factor of 1000 times less massive.

Next, take a net force that might be used to accelerate the massive 100 kg objects, and instead apply the same force to the 0.1 kg spring. The spring's acceleration will be 1000 times more than that of the massive objects, and would appear to move extremely fast.

Finally, if one stipulates that the spring does not accelerate or move very quickly, the net force on it would have to be rather small for that to be the case. To make calculations simple in high school and college freshman physics courses, we stipulate that this net force is zero. Though not rigorously true, it's a good enough approximation to:

1) calculate forces fairly accurately
and
2) learn some "building block" principles of how forces behave.

I would save concerns about relativity and quantum mechanics for more advanced physics courses. Learn these basics first.
 

1. What is the formula for calculating the net force on a massless body?

The formula for calculating the net force on a massless body is Fnet = ma, where Fnet is the net force, m is the mass of the body, and a is the acceleration.

2. How is acceleration related to the net force on a massless body?

Acceleration is directly proportional to the net force on a massless body. This means that as the net force increases, the acceleration of the body also increases.

3. How does the spring force affect the net force on a massless body?

The spring force, also known as the restoring force, is a force exerted by a spring when it is stretched or compressed. This force is directly proportional to the displacement of the spring, and it adds to the net force on a massless body, causing it to accelerate.

4. Can a massless body experience acceleration without any net force acting on it?

No, a massless body cannot experience acceleration without any net force acting on it. According to Newton's second law of motion, an object can only accelerate if there is a net force acting on it.

5. How does the direction of the net force affect the acceleration of a massless body?

The direction of the net force determines the direction of the acceleration of a massless body. If the net force is in the same direction as the body's motion, it will accelerate in that direction. If the net force is in the opposite direction, it will decelerate or change direction.

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