> > Versus the system K the relatively moving system K' is moving at .5 C
> >
[quoted text clipped - 33 lines]
>
> Paul Cardinale
You mean that a ball of insignificant mass traveling at .8 C hitting a wall
of very large mass traveling in the same direction at .5 C would result in
a velocity of 0 C ??
Is like saying that a little ball of glass that travels at 8 mt./s hitting a
heavy wall going at 5 mt/s in the same direction, after the impact would
stop ?????
Are you sure ???????
It looks like to me that the little ball would be bounced backwards at the
speed of 3 mt /s.
So would do a ball traveling at .8 C after hitting
the wall at .5 C, it should be bounced back at the speed of .3 C !!!!!
would you please verify once more ??, thanks
best regards
beda pietanza
Dirk Van de moortel - 28 Dec 2004 22:03 GMT
> > > Versus the system K the relatively moving system K' is moving at .5 C
> > >
[quoted text clipped - 46 lines]
> It looks like to me that the little ball would be bounced backwards at the
> speed of 3 mt /s.
That would be 2 m/s forwards.
See below.
> So would do a ball traveling at .8 C after hitting
> the wall at .5 C, it should be bounced back at the speed of .3 C !!!!!
[quoted text clipped - 4 lines]
>
> beda pietanza
Small ball mass m and velocity v before collision and v' after collision.
Big ball mass M and velocity V and V' after collision.
Positive velocities indicate movement to the right.
Negative velocities indicate movement to the left.
At the end I'll turn the big ball into a wall.
Conservation of momentum gives
m v + M V = m v' + M V'
Conservation of energy gives
1/2 m v^2 + 1/2 M V^2 = 1/2 m v'^2 + 1/2 M V'^2
Putting k = M/m this becomes
v + k V = v' + k V'
v^2 + k V^2 = v'^2 + k V'^2
Solving for v' and V' gives
v' = (2 k V + v - k v ) / (k+1)
V' = (k V + 2 v -V ) / (k+1)
An infinitely massive wall means infinite k, so taking the limits:
limit( k --> infinity, v' ) = 2 V - v
limit( k --> infinity, V' ) = V
Little ball has initial velocity v = 8 m/s
Big ball (the wall!) has initial velocity V = 5 m/s
After the collision, the wall keeps going at V'(limit) = 5 m/s,
and the little ball has v'(limit) = 2 V - v = 2 m/s, which is
positive, so still going forward.
Dirk Vdm
beda - 29 Dec 2004 18:34 GMT
> > > > Versus the system K the relatively moving system K' is moving at .5 C
> > > >
[quoted text clipped - 86 lines]
>
> Dirk Vdm
I thank you very much.
Looks like that in order to stop the ball should have a speed of 10
mt/s, taking the wall as reference the ball approaches it at 5 mt/s and
of course is bounced back at
-.5 mt/s versus to the wall, that makes the final speed of the ball 0
mt/s.
In my original post the ball (in the frame K)would travel at .8 C and
the wall at .5 C (at rest in the frame K'(K' moving at .5 C in the same
direction)).
After the ball hits the wall, SR tells us that the ball stops in the
frame K while travels back at -.5 C in the frame K'.
In K' the ball travel forth at .5 C hits the wall and comes back at -.5
C.
In K the ball travels forwards at .8 C hits the wall at .5 C and
stops.
And applying your approach using the wall as reference the ball is
travelling at .5 C approaching the wall that makes obvious that the
ball would be bounced back at - .5 C versus the wall that brinks the
ball to a stop versus the frame K, perfect, all fits.
I still want to make out what the Esynchro has to do with this result.
Anyway,.8 C versus .5 C in SR stands as 10mt/s versus 5 mt/s in low
speed classical mechanics.
Very grateful to you..
beda pietanza
Dirk Van de moortel - 30 Dec 2004 10:37 GMT
> > "beda pietanza" <beda-pietanza@libero.it> wrote in message
> news:IkkAd.6600$H%6.292827@twister1.libero.it...
[quoted text clipped - 117 lines]
> -.5 mt/s versus to the wall, that makes the final speed of the ball 0
> mt/s.
Yes, in the non-relativistic case, to make v' = 2 V - v zero and thus
stop the ball, v must be the double of V.
> In my original post the ball (in the frame K)would travel at .8 C and
> the wall at .5 C (at rest in the frame K'(K' moving at .5 C in the same
[quoted text clipped - 17 lines]
> Anyway,.8 C versus .5 C in SR stands as 10mt/s versus 5 mt/s in low
> speed classical mechanics.
Yes, and like 9.9999999999999972 m/s versus 5 m/s in SR
itself.
Ask yourself this... is there any reason why one would prefer
10 m/s over 9.9999999999999972 m/s ? How would you
measure the difference?
> Very grateful to you..
>
> beda pietanza
No problem.
I just gave this as a little showcase of the power of the
mathematical model we use to do physics.
Paul's explanation using the Galilean transformation leads
you to the same result directly, but of course it only works
in the case of an infinitely massive wall, and you don't get
the intermediate results of the heavy ball.
Dirk Vdm
Paul B. Andersen - 29 Dec 2004 09:56 GMT
>>>Versus the system K the relatively moving system K' is moving at .5 C
>>>
[quoted text clipped - 51 lines]
> of very large mass traveling in the same direction at .5 C would result in
> a velocity of 0 C ??
Yes.
> Is like saying that a little ball of glass that travels at 8 mt./s hitting a
> heavy wall going at 5 mt/s in the same direction, after the impact would
> stop ?????
No, because 0.8 c is very different from 8 m/s.
A ball going at 8 m/s would drop dead if it hits a wall going at 4 m/s.
> Are you sure ???????
>
> It looks like to me that the little ball would be bounced backwards at the
> speed of 3 mt /s.
Wrong.
See Dirk's response.
A somewhat simpler approach is to transform the speed to the wall-frame,
and then transform it back, using the Galilean transform since the speeds
are so low.
In the wall frame, the ball is approaching the wall with the speed 3 m/s,
and is bouncing back at the speed -3 m/s. Transformed back, the speed is
thus - 3 m/s + 5 m/s = 2 m/s
> So would do a ball traveling at .8 C after hitting
> the wall at .5 C, it should be bounced back at the speed of .3 C !!!!!
According to Galilean relativity, it would go at 0.2 c in the same direction.
According to SR, it will drop dead.
Paul