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Zs, to test or calculate?

A large contractor working on our site have told me yesterday that it is their policy not to live test final circuits where they cannot use a plug? In order to reduce risk, they will now only calculate Zs, on circuits where they would have to open an enclosure, such as FCU's and light fittings.
The control measures we insist are in place, are IP2X equipment, GS38 leads, two man rule with second man having resus training, among others. So I feel the risk has been reduced to as low as reasonably practicable. An d my instinct tells me that a measured Zs reading must be more accurate than a calculated one, since it will include all parallel paths under test.
The contractor is happy to live test distribution circuits, so it seems they want to pick and choose.
They also state that this is how things are now, and have worked at many different sites, Cross Rail, Heathrow, various MOD sites etc, and that they al accept this as common practice.

I like some opinions to find out what's going on out there on other sites. 
  • mapj1:

    A loop impedance test of the kind that uses the  50Hz AC supply and switches in a load and looks at the voltage drop will necessarily include all the same impedances, both real and imaginary, that  will appear in a real fault, as that too uses the AC supply.

     


    But how is that possible? The reactive component of voltage drop in the circuit being measured cannot be determined from an arithmetic subtraction of the voltage drop of the instrument test resistor from the supply voltage. As far as I understand it my MFT places a 59 ohm resistor as a dummy load, tries to establish the volt drop across it over a couple of half cycles and then determines the circuit “impedance” from the voltage difference between that and the supply voltage. Where the reactive component is pronounced surely that is not possible as the VD across the reactance is in quadrature.


  • Pencils can be truly wonderfull things ?
  • I know an electrician, now retired, who didn’t have his NICEIC renewal signed of by his assessor around fifteen years ago after a few clashes.


    One clash was when his assessor suggested he bought a non-trip loop tester to get more accurate loop test results on RCD protected circuits and he replied saying he had a pencil.


    On a personal note I still have my original Robin multifunction installation tester, the main reason I “upgraded” by buying a Megger non-trip loop tester to accompany it was the increasing number of RCDs being installed, now it seems all these years later I could have stuck with the Robin and a pencil.


     Andy Betteridge
  • It seems that nowadays it is acceptable across the board to calculate Zs.

    As an aside, I don't think of adding dead R1+R2 results to Ze as being the calculation approach - it's still all based on measurement even if done in parts. For me, calculation would be something like working out the impedance based on the cable length and tabulated resistance per metre - which might have been the approach in the old days when earth continuity would be verified with nothing more than a set of test lamps.

       - Andy.
  • A loop impedance test of the kind that uses the  50Hz AC supply and switches in a load and looks at the voltage drop will necessarily include all the same impedances, both real and imaginary, that  will appear in a real fault, as that too uses the AC supply.

    The accuracy problem is because   the test current is much lower than a likely fault current  (on a TN system anyway) the voltage drop caused during the test is fractions of a volt, and  if the mains is a bit bouncy for other reasons, as it often is if the supply is shared with loads that are switching, then the meter may mistake some of that voltage drop for the result of its own test load, so the results can be a bit 'fruit machine'.

      By keying the test load in and out in a psuedo-random sequence, and then looking at the average voltage droop and rise for each short part of that test, it is possible to cancel out and mitigate this noise problem, at least to a degree. Also when you are looking at PSSC of kA, then every milliohm starts to count, and the condition of test leads and their connectors starts to be a significant part of the reading, and beyond a certain point 'normal' meter  probes are not really good enough.


    Also I  have seen the effects of RCD cores that look inductive for small currents, but for  large fault would saturate and not current limit, give an over pessimistic impedance on a very low current (no trip) test. The clue is the Zs readings before and after the RCD are far more different than the DC resistance of the contacts would suggest. Still only tens of milliohms of change, but in some cases that may be misinterpreted as the difference between additional work needed, and not.
  • I am not convinced that the loop test does not measure impedance. Yes, the current used is DC but, as I understand it, a very short pulse is used so inductive effects should be measured too.

    I have also had great difficulty measuring the earth loop impedance of a main incomer, say 400A, because the dip in voltage caused by the brief current pulse was so small that it was masked by the normal spikes on a supply. I tried averaging several successive readings but as some of these were negative, I didn't trust the results. 

    I suspect that, to get a proper result, I needed a much beefier bit of test kit, the sort that would take 2 people to carry it.
  • As far as I know, the reactive component of impedance is not measured by a loop “impedance” tester anyway. Further, the accuracy is always questionable for various reasons. Having that margin of 0.8 Zs7671 as a maximum test value perhaps addresses most issues. A loop impedance on the wrong side of an mcb is worse than a fuse.
  • For circuits below say about 63 A, we don't worry about the reactance of the cable - see tables at the back of BS 7671. Most of the reactance is in the external loop, and that's why we would normally measure at least Ze or ZDB.


    Appendix 14 of BS 7671 advises that, under many circumstances, measurement prospective fault current in domestic installations is not necessary.


    For larger circuits, I agree there's perhaps something missing, but it's worth remembering that, due to potentially larger prospective fault currents / lower loop impedances, and especially where you are close to the transformer, the loop impedance or prospective fault current measurement itself may be inaccurate. For larger loads, and even final circuit disboards, there is no reason at all why a test socket-outlet specifically for prospective fault current and loop impedance measurement, with suitable backup protection could not be provided, just below the DB or built into MCCs etc. - this is part of the CDM process.


    Don't forget that Appendix 14 of BS 7671 advises that fused leads alone may not provide protection if backup protection at the point of measurement is not present.
  • Thanks for everyone's replies. It's good to get other opinions. It seems that nowadays it is acceptable across the board to calculate Zs. When I used to do a lot of testing, the contractor I worked for insisted on measured readings. That was the company line and therefore that is how I used to work. At that time a calculated Zs was seen as "lazy", so that is my mindset still. Companies are a lot more wary of risk these days, whereas then, you were just told to get on with it.

    One more nagging doubt though. If you measure with a loop tester, you are literally measuring the earth loop "Impedance". However, if you add r1+r2 which is "Resistance" to the Ze (or Zdb), then that calculation is actually "Impedance + Resistance"

    Looking at the Impedance triangle, we have Z= √R²+(Xl-Xc)², so clearly Z is going to be greater than R.

    This will only come into play if the circuit is actually operating and under load. For example a radial socket circuit with nothing plugged in, there will be no difference.  But if you are testing a circuit feeding inductive or capactive loads, then the difference will be more pronounced. In this case wouldn’t a measured Zs be accurate whereas the calculated Zs less so?

  • Method 1 (R1+R2) in the OSG and GN3 doesn't show the cpc being disconnected.

    Very good point Graham. I've certainly seen the c.p.c. and line 'choc blocked' together suggested somewhere (I'll have to rack my brains as to where now) - and was under the impression that it was frequently taught that way too - I've certainly seen it been done that way in practice. Good news if that's officially incorrect.

     
    Why would the impact of parallel paths differ between Method 1 to Method 2?

    I mean to suggest it would - just that disconnecting the c.p.c. from the Earth bar would eliminate some parallel paths (which I understood was the reason for the disconnection approach in the first place).


      - Andy.