Wave propagating along a string - Newton's 3rd Law

  • Thread starter Thread starter Jack3000
  • Start date Start date
  • Tags Tags
    Law String Wave
AI Thread Summary
The discussion centers on the application of Newton's Third Law to wave propagation along a string. When a wave travels, each point on the string exerts forces on adjacent points, creating a complex interaction of upward and downward forces. The tension in the string counteracts local curvature and seeks to restore the string to a straight line, which is essential for wave propagation. The initial disturbance from a hand movement generates a wave that reflects and continues due to the conservation of energy, even as damping forces eventually reduce the vibrations. Understanding these dynamics clarifies how waves behave in a string under tension and the role of forces involved.
Jack3000
Messages
1
Reaction score
0
wave propagating along a string -- Newton's 3rd Law

I'm a bit confused about the action-reaction forces (ie. Newton's Third Law) when a wave propagates along a string. I think I'm confused about a point not mentioned elsewhere in the forum.

Let's imagine the string is made up of many tiny particles, and that it carries a wave propagating in the right to left direction. A person holding the right end of the string rapidly displaces that end upwardly, then rapidly displaces that end back to its original position. Then if one point somewhere along the string (let us call it "x") waves upward, it places a force on the point just to its left (x+dx). By Newton's third law, wouldn't this point (x+dx) push on point "x" with an equal and opposite force?

It seems to me that such an equal and opposite force woud tend to return the string just behind the wave, to its original position. But I thought that it was the downward movement of the hand that returns the string to its original position?

Thanks!
 
Physics news on Phys.org
When you wish to understand how tension in a string can make a wave propagate, it is important to realize that the tension counteracts local curvature.
Another way of saying this, is that tension seeks to minimize the string length (i.e, seeking to reestablish the string as a straight line)
I'll post some calculations a bit later
 
"A person holding the right end of the string rapidly displaces that end upwardly, then rapidly displaces that end back to its original position. Then if one point somewhere along the string (let us call it "x") waves upward, it places a force on the point just to its left (x+dx). By Newton's third law, wouldn't this point (x+dx) push on point "x" with an equal and opposite force?"

Certainly!
(In the following, I will assume that the other end of the string is fixed to some wall)
In addition, (assuming, for the moment that x is at a local top), x exerts an upwards force on a point at (x-dx).
By Newton's 3.law, the point at (x-dx) also exerts a downward force on "x".

"It seems to me that such an equal and opposite force woud tend to return the string just behind the wave, to its original position."

No it does not!
As long as "x" is higher placed than "x+dx" and "x-dx", "x" experiences a net force downwards, i.e accelerates downwards, which means gaining downwards velocity.
What happens then at the moment at which "x", "x+dx", "x-dx" are all on a line?
Well, "x" has downwards velocity, wheras "x+dx" and "x-dx" have upwards velocity.
Even though at that moment "x" does not experience a net vertical force,
it will proceed downwards, and will begin experience a net, upwards force (i.e, slowing down).

"But I thought that it was the downward movement of the hand that returns the string to its original position?"

The above argument shows, that if you disturb a string , you will set up a wave signal that will continue indefinitely, that will reflect at the other end, return, and reflect again..
Essentially, the initially imparted kinetic and potential energies will swith about, according to conservation of energy.

If we have both ends fixed for a vibrating string, the vibration will eventually die out as a result of frictional forces/air resistance (i.e, damping).
 
I'm not altogether sure if I have answered what you wanted an answer to here..
 
TL;DR Summary: I came across this question from a Sri Lankan A-level textbook. Question - An ice cube with a length of 10 cm is immersed in water at 0 °C. An observer observes the ice cube from the water, and it seems to be 7.75 cm long. If the refractive index of water is 4/3, find the height of the ice cube immersed in the water. I could not understand how the apparent height of the ice cube in the water depends on the height of the ice cube immersed in the water. Does anyone have an...
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top