On Thursday, May 1, 2025 at 10:17:19 PM UTC-6 Alan Grayson wrote:

On Thursday, May 1, 2025 at 8:42:45 PM UTC-6 Brent Meeker wrote:

On 5/1/2025 7:25 AM, Alan Grayson wrote:

      On Wednesday, April 30, 2025 at 11:06:07 PM UTC-6 Brent Meeker wrote:

             On 4/30/2025 5:54 PM, Alan Grayson wrote:

                    On Wednesday, April 30, 2025 at 2:41:43 PM UTC-6 Brent 
Meeker wrote:

                            On 4/30/2025 4:29 AM, John Clark wrote:

                                  On Tue, Apr 29, 2025 at 8:09 PM Brent 
Meeker <[email protected]> wrote:


                                       *>> If you place two macroscopic 
conductive plates close to each other the Casimir Effect will              
                                 cause the two plates to attract each 
other; this occurs regardless of if you make any                            
                               measurements or not. It happens because 
there are fewer virtual particles between the two                          
                   plates than there are outside the plates. And virtual 
particles exist because it's impossible                                    
           for the energy in the electromagnetic field to be exactly zero 
for any arbitrary length of                                                
     time;  **and the shorter the time the greater the deviation from zero 
it's likely to be.  JC*


*>That's why the qualification about measure like interactions.  The two 
conductive plates exclude longer wavelengths. *


*Yes.*

* > I don't recall that the effect depended on duration. *


*Heisenberg's uncertainty principle is not just about the relationship 
between momentum and position, it also insists there is a similar 
relationship between energy and time; the shorter amount of time the 
greater the random variation from a zero value there is. *


In quantum mechanics *energy* and the *time per unit change of a variable* 
are conjugate variables. So they satisfy an Heisenberg uncertainty 
relation, often written $\Delta E \Delta t \geq \hbar$ . This is sloppy 
though and not quite right. What is right is given any operator $A$ and the 
Hamiltonian $H$ defining the time evolution of $A$, then $\Delta A \Delta H 
\geq \frac{1}{2} \hbar [d<A>/dt]$ . In this case I don't see what is the 
time per unit change in the expected value of the energy density between 
the plates?  The plates are assumed stationary. 

Brent


In the time-energy form of the HUP, what is the role of time as an 
operator? What does *time per unit change of a variable* mean? Which 
variable is referenced? About virtual particles; aren't they elements of a 
perturbation expansion and thus not to be considered real since those terms 
violate conservation of energy? TY, AG

That's why I include the equations (although I see they didn't get 
converted to display).  It can be any variable whose change is encoded by 
the Hamiltonian, A and H respectively in the equation.  It doesn't have 
anything to do with how you might solve the equations; which is where 
perturbation expansions and virtual particles enter.

Brent


Can you give some examples of what A could be, and mustn't A be an 
*operator,* not a variable, that commutes with H?

*Sorry, I meant that the operator A does NOT commute with H. AG *

Yes, A is an operator, but it doesn't commute with H.  That would imply the 
variable measured by A is constant in time.  The time per unit change in 
the expected value of the variable is the inverse of [d<A>/dt].


*What is d? Can you give one or two specific examples of A? I thought the 
HUP is applicable only for non-computing operators. Am I mistaken? AG*

If your claim is correct, ISTM that Clark cannot apply the Time-Enegy form 
of the HUP to make his claim about the Casmir Effect. Do you agree? AG

I don't know.  I don't understand the proposed role of time. 


*Same here, and more generally, so I find applying the time-energy form of 
the HUP dubious at best, but this is how the Casmir Effect is presumably 
established in quantum EM theory.  If you recall, Bruce Kellet, an 
excellent physicist IMO, claimed the **Casmir Effect can fully accounted 
for classically. He also vehemently denied that virtual particles are real 
due to energy considerations, given that virtual particles violate energy 
conservation. AG*

It doesn't seem to have anything to do with conducting plates.  Perhaps he 
means the period of EM fields filling the gap between the plates.  Those of 
long period being excluded from between the plates would thereby remove 
their repulsive pressure and leave an unbalanced compressive pressure.

*Hopefully, Clark can explain what he meant. AG*


Brent

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