For RCD protected circuits the EFLI can be a lot higher than was traditionally permitted (1667 ohms is bandied around).
An EFLI of 7,667Ω is low enough for a 30mA RCD to respond to an L-E fault. However, a Ze above 200Ω is not considered acceptable for a TT electrode (and ≤100Ω really desirable),
I'm not ignoring the possibility of LN faults my query is about exactly that.
Apologies. As should be apparent from what I went on to write, that was a typo (noe corrected). I should have typed "L-E fauklts".
Ok fine but the point is the graph has to be looked up, it wont slot into a cell in excel without lots of hassle!
You don't seem to understand why the magic formulae you so much want could not be produced. What matters is how real OPDs actually perform, and that can only be determined empirically (as per the published graphs). Any formulae one attempted to produce on a theoretical basis would almost certainly fail to reflect accurately how the real-world devices actually perform.
It's the equation from 434.5.2. Yes values of K are for up to 5 seconds. If you had the actual disconnection time you would be able to compare it with the maximum value calculated from the equation. I guess values of k for faults longer than 5s are hard to come by but I am still interested to know how long a fault will take to clear if it is under or around 5 seconds.
Again, you don't seem to understand. It's not just that values of k for longer duration fault currents "are hard to come by". The point/problem is that the equation itself (which, at best, is an approximation) ceases to be valid for currents of longer duration. It is an "
adiabatic" equation - which means that it only applies in the very simple situation in which heat is produced (current flows) for such a short period of time that there is no time for any significant 'movement' of heat to occur. If the duration of heat production (current flow) becomes more than a few seconds (usually said to be about 5s), heat will start moving from the conductors, and the calculation becomes dramatically more complicated, because it depends upon such factors as the geometry of the cable, the properties of the insulation and sheath, the orientation and path of the cable, the ambient conditions etc. etc. etc.
Kind Regards, John