Richard Haynes wrote:
> 
> Doug,
> Thanks for adding your important two cents. Could you show us an example
> with the necessary conversions numbers. Also there is the concept of
> equilivalents/mole where the number of equivalents is effectively the
> valence, i.e. 2 for Cu(+2). There are some cases where n is not an even
> intergal. All is all a dimensional analysis must yield a dimensionless
> number in the exp(E or H or F).
> Thanks
> Richard Haynes


Sure,  and I would certainly invite any corrections. 

One over-riding theme when using equations is to be 
sure of the assumptions by which they have been deduced.  
The Arrhenius equation is a good approximation for simple 
atoms/molecules.  As one moves away from simple atomic 
structures to more complex molecules, the idea of "heat" 
has to change.  Complex atomic structures no longer bang 
into one another more so at higher temps than lower. 
They begin to do all sorts of strange things like twist, 
bend, longitudenally vibrate, etc ...  In other words, 
different modes of displaying heat come about. 

Alright, now that everyone's gone to sleep, here we go. 

Using  Arrhenius Equation = exp[ (Ea/R)*(1/T1 - 1/T2) ] 
where  

Ea = Activation Energy 

 * Note: The less the value, the less sensitive to temp; 
         the greater the value, the more sensitve to temp. 

R  = Gas Constant
T  = Temperature in degrees Kelvin 

How we pick the units of R determines everything else as 
far as units go.  One form of the gas constant is: 

R (Gas Constant) = 8.3144 J/mol*K  and 1/R = 0.1203 

Thus,  AE = exp[0.1203*Ea*(1/T1 - 1/T2)] 

This means that if Ea is divided by R, the units K must 
remain in the numerator to cancel the K in the denominator 
from the (1/T1 - 1/T2) factor.  This will leave the final 
exponent dimensionless.  Thus, Ea should be in the units J/mol.  
This form (J/mol) is very different in implications than 
simply Joules. 

Changing this constant to units that have calories involves 

   1 calorie = 4.184 Joules 

R (Gas Constant) = 1.9872 J/mol*K  and 1/R = 0.50322 

Thus,  AE = = exp[0.50322*Ea*(1/T1 - 1/T2)] 

This means Ea is now in the units cal/mol. 

The form of Arrhenius with which I'm familiar uses electron volts 
(eV's) as units.  So, using the conversion 

   1 eV = 96.485 kJ/mol 

leaves  R = 8.6172E-5 and  1/R = 11,604.56557 

Thus,  AE = = exp[11,604.5656*Ea*(1/T1 - 1/T2)] 

This means Ea is now in the units eV/mol. 
   Ea = 0 eV/mol -> temp has no effect. 
   Ea = 1 eV/mol -> temp has alot of an effect. 

Some semi-mfrs use 0.4 or 0.5 for estimates with 
CMOS and higher numbers for 0.6 or even 0.7 for 
BJTs.  It is important to note that since there
is such a mix of semi-conductor material in any 
device, it is better to estimate, then empirically 
derive (as long as you have enough sampling) the 
Ea specific to the product.  That will take some 
time. 

Here's a sample of how they all work out so that 
the same AF (acceleration factor) comes out the 
same no matter which version of Arrhenius you 
choose to use. 

-------------------------------------------------------
**** INPUTS *** 
-------------------------------------------------------
Test time at T1 =  16,006 hours
                   666.92 days  (interesting) 
                    95.27 weeks 
                     1.83 years 

T1              =      30    C (equation converts to K) 
T2              =      50    C    "        "      "  " 

Ea  eV/mol      =       0.6
    J/mol       =   57891.00
    cal/mol     =   13900.00

-------------------------------------------------------
*** OUTPUT ***
-------------------------------------------------------
AF = 4.1490     :   3857.79 hours 
                     160.74 days 
                      22.96 weeks 
                       0.44 years 

-------------------------------------------------------
-------------------------------------------------------

Regards,  Doug

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