Converting JJ Thomson's q/m Units to Modern Standards

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This discussion focuses on converting JJ Thomson's original q/m measurements from electrostatic units to modern SI units. Thomson's initial value of approximately 1.76x10^7 electrostatic units is now accepted as 1.75882001076(53)×10^11 C/kg. The conversion process involves recognizing that Thomson likely used the electromagnetic charge unit, specifically the absolute Coulomb, leading to a derived value of 5.70 × 10^-8 g abC^-1. The discussion emphasizes the importance of using rationalized Gaussian units or SI units for accurate scientific communication.

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How to convert from the units used to report q/m by JJ Thomson to the units used in the now accepted form of q/m.
Summary: How to convert from the units used to report q/m by JJ Thomson to the units used in the now accepted form of q/m.

Referencing the below paper... The q/m measurement was first done in 1897 and reported by JJ Thomson. Numerous others measured the same in the early 1900's. The paper below gives a chronicle of those measurements which appear to converge on a value of 1.76x10^7 and they refer to units of this measurement as "electrostatic units". Today's accepted value is different by several orders of magnitudes; 1.75882001076(53)×10^11 C/kg. This leads me to believe that "electrostatic units" are not the same as C/kg but I cannot find a source that can confirm the conversion. It appears that one can just multiply by 10,000 but that is conjecture... I really would like to have a source.

https://www.cs.princeton.edu/courses/archive/fall05/frs119/papers/smith97_thomson.pfg.pdf
 
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It's obviously not in electrostatic units. In the original paper

https://doi.org/10.1080/14786449708621070
Thomson quote the value for ##m/e## of being around ##0.5 \cdot 10^{-7}## (without giving a unit; he'd not pass the intro lab in our university today ;-)). Let's see which units he most probably has used. In matters of absolute values the SI is the save ground to start from: ##m/e \simeq 5.70 \cdot 10^{-12} \text{kg} \, \text{C}^{-1}##. Now in science even in England masses were measured in grams. So we have ##m/e \simeq 5.70 \cdot 10^{-9} \text{g} \, \text{C}^{-1}##. Now there's only a discrepancy of a factor of 10.

Checking Wikipedia for historical units of electromagnetism, we find that thus he must have used the electromagnetic charge unit, the socalled absolute Coulomb. Now ##1 \; \text{C} \widehat{=}0.1 \, \text{abC}##, i.e., we have ##m/e \simeq 5.70 \cdot 10^{-8} \text{g} \, \text{abC}^{-1}=0.570 \cdot 10^{-7} \text{g} \, \text{abC}^{-1}## in accordance with Thomson's measurements.

Unfortunately the English Wikipedia has not that very useful table the German Wikipedia has:

https://de.wikipedia.org/wiki/Elektromagnetische_Maßeinheiten#Elektromagnetische_Einheiten_in_verschiedenen_Systemen

The most convenient system of units for electromagnetism, used today in theoretical high-energy physics, are the rationalized Gaussian units, also known as Heaviside-Lorentz units (usually taken in natural units, where ##\hbar=c=1##. In the letter form it's identical with the SI setting ##\mu_0=\epsilon_0=1##. If it comes to concrete numbers, the one and only system is of course the modern SI units with all the (now exactly defined!) values for the fundamental constants left intact.
 
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Makes complete sense! Thank you kindly for your effort and well written response.
 

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