The principle of calibration (how does a reference or DMM agree with a better one?) and the quest to distribute the SI representation is clear to me.
My cheapo-no-magic reference aka "V
bs" ( Volt babysitter) was compared to a volt-nuts 4 other references (including a LTZ in a 3458 which was used for the 24h, 31h, 1 Week and noise experiments) that haven't been calibrated relative to a cal-lab for a while but their behaviour is closely compared to each other regularly. (If one of them wants to go for a ride voltagically speaking, you wouldn't realise if it is alone, but it will visibly differ from its siblings!)
My V
bs behaves closely like that cluster, how it differs in the long term I will see, got it back yesterdays from the first experiments. Now the V
bs is on its own for say one or three months...
What I meant with my last question is that it is increasingly getting harder to tell who is the reason for a deviation, the noise and drift of the V
bs is no longer easy to discern from that of the 3458A.
Also, in October iirc I will get a 34401A at work back from the Böblingen Cal lab of Agilent. This has not the greatest long-term-stability, but immediately after arriving it will be reasonable close to what they measured against their traceable references. Knowing the instruments error as noted by the lab, taking some readings from the babysitter volt abusing the 34401As gratuitous extra digits coming out of GPIB will give a cloud of datapoints for you know what... the V
Agilent vs. V
bs and later V
bs against V
volt-nut and also V
bs vs V
Quarks .
But I have to tell, the main reason for the LTZ reference is the predecessor, a REF102-based 10V, did not comply with my minimum requirement: Measure it at work, stuff it in the backpack, take it home and back to work the next day, measure again, delta only at the last digit. This one does so, after travelling much more. Now I can trust it for testing the DMM at home.
Greetings,
Hendrik