Interesting question. Since the frequency of a photon increases as it gains 
energy on the way into the hollow gravitational sphere one might expect time to 
speed up for it.  If it is allowed to pass through another hole on the other 
side the time rate would return to the original value once it reaches the same 
distance away from the sphere in that direction.

This appears to be a paradox of some type. It is common to speak of time 
slowing down, but a bit strange to think of it as speeding up under some 
conditions. Wonder where I went wrong with this arguement?

Perhaps the photon could bounce around inside the hollow reflective sphere for 
a long time before exiting an offset hole. Since its frequency is higher while 
trapped inside it appears that many more cycles of oscillation would take place 
for this photon than for a brother photon reflecting between two mirrors 
outside the sphere for the same elapsed time.  Would a phase detector comparing 
the two show anything?

Dave

 

 

 

-----Original Message-----
From: H LV <[email protected]>
To: vortex-l <[email protected]>
Sent: Fri, Dec 9, 2016 1:42 pm
Subject: Re: [Vo]:Newtonian Gravity and General Relativity inside a spherical 
shell.







On Wed, Dec 7, 2016 at 4:04 PM, Stephen A. Lawrence <[email protected]> wrote:

          
    Well known result -- gravitational time dilation has to do with the    
gravitational potential, not the strength of the field.
    




 

    Simple gedanken:  Drop a rock through a slender shaft into a    spherical 
hollow cut out of the center of a spherical planet.  The    rock has more 
kinetic energy when it gets to the center of the    planet.
    
    Turn the rock (along with its kinetic energy) into photons, and beam    
them back up the shaft.  At the top of the shaft, catch the beam and    turn it 
back into a rock.
    
    The rock must have the same mass at the end as it had to start with    (or 
something's very wrong), which is smaller than the mass it had    at the bottom 
of the shaft (due its additional kinetic energy which    shows up as a mass 
excess).  This can only be true if the beam of    light was redder at the top 
of the shaft than the bottom.     So, there must have been a gravitational 
red-shift as the light    climbed the shaft.
    
    So, the frequency of the light at the top of the shaft must    be lower 
than the frequency at the bottom of the shaft.
    
    But the total number of wave crests in the beam of light    can't change.  
(You can count them, using appropriate equipment; in    that sense they behave 
like marbles.)  A certain number of wave    crests in the beam entered the 
shaft at the bottom; the same number    of wave crests must have come out the 
top.
    
    So, if the frequency measured by an observer at the top of    the shaft is 
lower than the frequency measured at the bottom    of the shaft, the wave 
crests must have taken more time to exit the    top of the shaft than they took 
to enter the bottom of the shaft,    and so, time must be passing faster for 
the observer at the top      of the shaft.
      
    
    
On 12/07/2016 12:53 AM, H LV wrote:
    
    
      
        
According to the shell theorem  the          gravitational force on a test mass 
inside a hollow sphere is          every where zero. This paper argues that 
this situation is not          equivalent from the standpoint of General 
Relativity to the          situation where gravity falls to zero far outside 
the sphere.          They conclude that General Relativity predicts that a 
clock          located inside a hollow sphere should run slower than a clock    
      located outside the hollow sphere. (By contrast most people          are 
familiar with the fact that General relativity predicts a          clock should 
run faster as the force of gravity approaches          zero far from a 
gravitational body) This could provide a          laboratory test of Newtonian 
gravity which predicts that both          clocks should run at the same rate. 
          
          
          https://arxiv.org/pdf/1203.4428.pdf
        
        

        
        

        
        
Harry
      
    
    
  





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