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| From | "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> |
|---|---|
| Newsgroups | sci.physics.research |
| Subject | Re: Newton e Hooke |
| Date | 2025-02-17 08:19 +0000 |
| Message-ID | <m1g9ofFcmisU1@mid.dfncis.de> (permalink) |
| References | (2 earlier) <vn34df$2to44$1@dont-email.me> <m132snF94igU1@mid.dfncis.de> <voloqi$3374b$1@dont-email.me> <m1dng8FkasU1@mid.dfncis.de> <vot1s2$lj72$1@dont-email.me> |
In article <m1dng8FkasU1@mid.dfncis.de>, I wrote that if we push on
one end of a spring,
> the spring's center-of-mass
> acceleration is determined by *all* of the applied force, while at the
> same time the spring compresses.
and I worked this out in detail for a simple model system.
I neglected to point out that there's actually a much simpler way of
coming to this same conclusion: simply apply conservation of momentum
to the spring.
That is, consider the spring's total (horizontal) linear momentum p.
Since there's an external force F pushing the spring to the right, p
must change according to Newton's 2nd law (dp/dt = F), i.e., the spring's
center of mass must be accelerating to the right at an acceleration
a = F/m_total.
The fact that the spring also has a bunch of internal dynamics isn't
relevant here -- we ony consider the spring's total linear momentum,
and the (horizontal) external force acting on the spring.
In fact, this argument is still true if there's no spring at all, just a
pair of (unconnected) point masses at the ends of the "spring". That is,
if we apply a force F to one mass, leaving the other mass stationary
(i.e., F is applied to mass #1, and there is no force applied to mass #2),
the center-of-mass of the two masses (at position xc = (x1 + x2)/2)
accelerates with an acceleration
ac = (a1 + a2)/2
= (F/m + 0)/2
= F/(2m)
= F/m_total
even though there the force is only pushing on one of the two masses.
In article <vot1s2$lj72$1@dont-email.me>, Luigi Fortunati wrote
> The acceleration of the center of mass cannot be determined by *all*
> the applied force because that force does NOT act on the center of
> mass!
For the momentum argument I gave above, it doesn't matter where the
applied force acts. We only care that it's an external force applied
to *somewhere* in the system of interest (the spring).
Luigi also wrote
> If you refuse to watch my animation https://www.geogebra.org/m/mrjtyuwk
> you cannot notice that the applied force Fa (black) acts on point A"
> and, before it can reach C, it must confront the opposing blue force.
Forces don't "reach" points or "confront" other forces. Forces (only)
act on, or are applied to, or push/pull on, objects or points on those
objects.
> The question is simple: does the opposing blue force in my animation
> exist or not?
Yes, there is a reaction force of magnitude F pushing left on the hand.
This force is pushing on the hand, not on the car, so it doesn't affect
the car's motion.
--
-- "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com>
(he/him; currently on the west coast of Canada)
"Every young man is prone to be misled by the suggestions of his
own ill-founded ambition which he mistakes for the promptings
of a secret genius, and thence dreams of unrivaled greatness."
-- Ralph Waldo Emerson
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Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-01-26 08:51 -0800
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-01-30 08:42 +0000
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-04 23:47 -0800
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-10 22:25 -0800
Re: Newton e Hooke "Jonathan Thornburg [remove color- to reply]" <dr.j.thornburg@pink-gmail.com> - 2025-02-12 08:02 +0000
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-14 08:09 +0000
Re: Newton e Hooke "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> - 2025-02-16 08:55 +0000
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-16 10:42 -0800
Re: Newton e Hooke "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> - 2025-02-17 08:19 +0000
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-17 22:45 -0800
Re: Newton e Hooke Tom Roberts <tjoberts137@sbcglobal.net> - 2025-02-18 08:23 +0000
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-16 10:42 -0800
Re: Newton e Hooke "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> - 2025-02-17 08:19 +0000
Re: Newton e Hooke "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> - 2025-02-18 08:23 +0000
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-20 07:56 +0100
Re: Newton e Hooke Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-22 18:13 +0100
inelastic collision (was: Re: Newton e Hooke) "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-red.com> - 2025-02-26 08:02 +0000
Re: inelastic collision (was: Re: Newton e Hooke) Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-02-28 14:44 -0800
Re: inelastic collision (was: Re: Newton e Hooke) "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> - 2025-03-01 09:18 +0000
Re: inelastic collision (was: Re: Newton e Hooke) Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-03-03 08:09 +0000
Re: inelastic collision (was: Re: Newton e Hooke) Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-03-12 12:37 +0000
Re: inelastic collision (was: Re: Newton e Hooke) Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-03-16 09:28 +0000
Re: inelastic collision (was: Re: Newton e Hooke) Luigi Fortunati <fortunati.luigi@gmail.com> - 2025-03-16 21:28 -0700
Re: inelastic collision (was: Re: Newton e Hooke) "Jonathan Thornburg [remove -color to reply]" <dr.j.thornburg@gmail-pink.com> - 2025-03-02 09:14 +0000
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