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Hello im currently doing the 2391 online I have failed 4 times but I realise there are variations to the voltage drop calculation could someone help me to know what the variations are to the voltage drop calculation I know the basic 1 thats fine but its the other ways for instance multiplying or dividing by 4 I have seen
 
Hello im currently doing the 2391 online I have failed 4 times but I realise there are variations to the voltage drop calculation could someone help me to know what the variations are to the voltage drop calculation I know the basic 1 thats fine but its the other ways for instance multiplying or dividing by 4 I have seen
Hi Mark. When you say the basic one, which one do you mean?
 
For circuits smaller than 25mm², there really is only one equation:

V(drop) = [tabulated VD] * L * Ib / 1000

The tabulated voltage drop is in millivolts per amp per metre, which is a fixed value for a particular size and type of cable. Multiply by the length L to get the total drop per amp along the length of the cable, then multiply by the design current Ib which is the maximum current that will flow under normal operating conditions. Then, because the tabulated value is in millivolts per amp per metre, the result would be in millivolts, so divide by 1000 to get volts.

If you consider that the tabulated voltage drop in mV/A/m is more or less a representation of its resistance in ohms per metre (R=V/I) then the voltage drop equation is an application of ohm's law: V (drop) = I (load) * R (cable). So it follows that there can really only be one equation at least where resistance is the main cause of drop, as it is in smaller cables. Once you get into very high current AC circuits, the reactance starts to become a significant factor and you have to consider that separately to the resistance, but I believe that is beyond the scope of your exam questions.

I am not sure whether your questions involve a mixture of 3-phase and single-phase circuits, but care is needed when calculating the VD to the end of a single-phase circuit supplied by a 3-phase submain. For a balanced 3-phase load, the VD relates to the line-line voltage, not the line-neutral voltage. The easiest way to deal with this is to convert the drop in each section into a percentage and add. So a 3-phase submain with 6V drop contributes 6/400 * 100 = 1.5%, while a single-phase final with 5.75V drop contributes 5.75/230 * 100 = 2.5% These can be added to give 4% total drop.
 
Last edited by a moderator:
mV/A/m / Length / Amps div 1000

volt drop like 9.5v max. if its change let me know its all from memory.

not sure what you mean by 4. 4 is for ring mains.

R1 + R2 / 4 = ring/ all same at sockets.
 
I was about to complain that @moose was breaking a number of laws of physics there, when I noticed some gobbledegook in my own post #4. Perhaps a mod can change it or let me edit the post: para 1, 'tabulated value is in millivolts per amp per metre,'
 
I was about to complain that @moose was breaking a number of laws of physics there, when I noticed some gobbledegook in my own post #4. Perhaps a mod can change it or let me edit the post: para 1, 'tabulated value is in millivolts per amp per metre,'
Edited.
 
5% with the exception of lighting which is

For circuits smaller than 25mm², there really is only one equation:

V(drop) = [tabulated VD] * L * Ib / 1000

The tabulated voltage drop is in millivolts per amp per metre, which is a fixed value for a particular size and type of cable. Multiply by the length L to get the total drop per amp along the length of the cable, then multiply by the design current Ib which is the maximum current that will flow under normal operating conditions. Then, because the tabulated value is in millivolts per amp per metre, the result would be in millivolts, so divide by 1000 to get volts.

If you consider that the tabulated voltage drop in mV/A/m is more or less a representation of its resistance in ohms per metre (R=V/I) then the voltage drop equation is an application of ohm's law: V (drop) = I (load) * R (cable). So it follows that there can really only be one equation at least where resistance is the main cause of drop, as it is in smaller cables. Once you get into very high current AC circuits, the reactance starts to become a significant factor and you have to consider that separately to the resistance, but I believe that is beyond the scope of your exam questions.

I am not sure whether your questions involve a mixture of 3-phase and single-phase circuits, but care is needed when calculating the VD to the end of a single-phase circuit supplied by a 3-phase submain. For a balanced 3-phase load, the VD relates to the line-line voltage, not the line-neutral voltage. The easiest way to deal with this is to convert the drop in each section into a percentage and add. So a 3-phase submain with 6V drop contributes 6/400 * 100 = 1.5%, while a single-phase final with 5.75V drop contributes 5.75/230 * 100 = 2.5% These can be added to give 4% total drop.
I understand the millivolts times length times ib I get that but some calculations im looking at you apply the 1.2 factor some is just ohms law thats needed and I'm struggling to differciate between the 2 and aswell the transposing is a bit confusing
 
I'll try to explain as I understand it:

At the origin of a single phase installation, you have a Line at 230V, and a Neutral at 0V - a potential difference of 230V.

Let's build a simple circuit - 10m of 2.5mm² T+E feeding a heater pulling 13A. That 13A will flow from the origin, through 10m of line conductor, through the heater, through 10m of neutral conductor back to the origin.

The bulk of the circuit resistance is in the heater, so the bulk of the potential difference will be across the heater. But the circuit conductors have a small resistance too, so there will be a small potential difference across the 10m of line conductor, and across the 10m of neutral conductor. Added together, this potential difference is the 'voltage drop'.

From the OSG, p196;
1m of 2.5mm² copper conductor has a resistance of 0.00741ohms at 20 deg C.
Therefore 20m would be 0.00741 X 20 = 0.1482ohms at 20 deg C.

The resistance of a conductor increases as it gets warmer, so we want to calculate the voltage drop at the maximum operating temperature of the conductor, when the resistance, and therefore voltage drop would be at its greatest. For T+E this is 70 deg C. A conductor at 70 deg C will have roughly 1.2 times the resistance of a conductor at 20 deg C.

So, 0.1482ohms X 1.2 = 0.17784ohms at 70 deg C.

V=IR
V = 13 X 0.17784
V = 2.31192V This is your voltage drop for the circuit.

Let's check that it tallies with the other method. From OSG P161:

1m 2.5mm² T+E has a VD of 0.018V/A/m. That's the VD for both line and neutral conductors, at 70 deg C.

0.018 X 13 X 10 = 2.34V/A/m

More or less the same, a very slight difference I expect due to rounding.

Note that I prefer to always work with volts rather than millivolts, which i think can confuse calculations sometimes.
 
I think @Pretty Mouth has hit on what the OP means by different formulas, i.e. calculating the VD from the tables at design stage, vs. verifying it during testing.

The method we've all given is convenient for calculating it at design stage where you know the length of the cable, so can easily use the VD figures from the table which apply to a cable under operating conditions.

If you are testing an installation and want to confirm the VD is in limits, you probably won't know the length of the circuit but you can measure its resistance, R1 + Rn. When you measure it, it's not energised, so the conductor will be at room temperature (typically 20°C) instead of maximum working temperature (typically 70°). If you apply ohms law to the measured resistance: VD = (R1 + Rn) * Ib you will get a figure for drop at room temperature, whereas it is necessary to check it would be OK at working temperature because the resistance of copper rises by about 0.39% per degree centigrade. This equates to a factor of 1.2 between room temp and working temp.

Multiplying the resistance measurement by 1.2 gives VD = (R1+Rn) * 1.2 * Ib

In a sense it is really the same calculation, you are just correcting the measurement for the fact that you cannot measure using a normal resistance meter while the circuit is loaded. Of course there might be situations in which the temperature correction factor of 1.2 does not apply. For example, a cable run in a cool location carrying only a small fraction of its rated Iz, might never exceed 30°C. A cable operating at a high temperature (MI in a blast furnace?) might need a greater correction factor.
 
For the divide by 4 thing on a ring: You've measured the total resistance of the wire in the ring.
Taking a socket exactly half way around the ring, it has only half the total length of this wire going to it, so half the resistance = divide by two.
But, you also have two wires in parallel going to this socket, so to find the combined resistance of them, you divide by two again.
Divide by two, then divide by two = divide by four.
 
Note that I prefer to always work with volts rather than millivolts, which i think can confuse calculations sometimes.

I'm the opposite. I use mV/m x A x L to get VD in mV, e.g. 2340mV. then just add a dec.pt. after the "2". saves a fat finger error when using a calculator.

and i disagree with the 1.2. factor when the magnitude of the cable load will not take it anywhere near 70 deg. in some cases this could be a major saving in cable cost.
 
I think @Pretty Mouth has hit on what the OP means by different formulas, i.e. calculating the VD from the tables at design stage, vs. verifying it during testing.

The method we've all given is convenient for calculating it at design stage where you know the length of the cable, so can easily use the VD figures from the table which apply to a cable under operating conditions.

If you are testing an installation and want to confirm the VD is in limits, you probably won't know the length of the circuit but you can measure its resistance, R1 + Rn. When you measure it, it's not energised, so the conductor will be at room temperature (typically 20°C) instead of maximum working temperature (typically 70°). If you apply ohms law to the measured resistance: VD = (R1 + Rn) * Ib you will get a figure for drop at room temperature, whereas it is necessary to check it would be OK at working temperature because the resistance of copper rises by about 0.39% per degree centigrade. This equates to a factor of 1.2 between room temp and working temp.

Multiplying the resistance measurement by 1.2 gives VD = (R1+Rn) * 1.2 * Ib

In a sense it is really the same calculation, you are just correcting the measurement for the fact that you cannot measure using a normal resistance meter while the circuit is loaded. Of course there might be situations in which the temperature correction factor of 1.2 does not apply. For example, a cable run in a cool location carrying only a small fraction of its rated Iz, might never exceed 30°C. A cable operating at a high temperature (MI in a blast furnace?) might need a greater correction factor.
Thank you very much what I'm gonna do im gonna go through past papers and apply this and see how I get on I will give feed back thanks
 
I think @Pretty Mouth has hit on what the OP means by different formulas, i.e. calculating the VD from the tables at design stage, vs. verifying it during testing.

The method we've all given is convenient for calculating it at design stage where you know the length of the cable, so can easily use the VD figures from the table which apply to a cable under operating conditions.

If you are testing an installation and want to confirm the VD is in limits, you probably won't know the length of the circuit but you can measure its resistance, R1 + Rn. When you measure it, it's not energised, so the conductor will be at room temperature (typically 20°C) instead of maximum working temperature (typically 70°). If you apply ohms law to the measured resistance: VD = (R1 + Rn) * Ib you will get a figure for drop at room temperature, whereas it is necessary to check it would be OK at working temperature because the resistance of copper rises by about 0.39% per degree centigrade. This equates to a factor of 1.2 between room temp and working temp.

Multiplying the resistance measurement by 1.2 gives VD = (R1+Rn) * 1.2 * Ib

In a sense it is really the same calculation, you are just correcting the measurement for the fact that you cannot measure using a normal resistance meter while the circuit is loaded. Of course there might be situations in which the temperature correction factor of 1.2 does not apply. For example, a cable run in a cool location carrying only a small fraction of its rated Iz, might never exceed 30°C. A cable operating at a high temperature (MI in a blast furnace?) might need a greater correction factor.
Thanks another I will apply this through my revision and give you feed back I've got 10 days till test so fingers crossed
 
I'll try to explain as I understand it:

At the origin of a single phase installation, you have a Line at 230V, and a Neutral at 0V - a potential difference of 230V.

Let's build a simple circuit - 10m of 2.5mm² T+E feeding a heater pulling 13A. That 13A will flow from the origin, through 10m of line conductor, through the heater, through 10m of neutral conductor back to the origin.

The bulk of the circuit resistance is in the heater, so the bulk of the potential difference will be across the heater. But the circuit conductors have a small resistance too, so there will be a small potential difference across the 10m of line conductor, and across the 10m of neutral conductor. Added together, this potential difference is the 'voltage drop'.

From the OSG, p196;
1m of 2.5mm² copper conductor has a resistance of 0.00741ohms at 20 deg C.
Therefore 20m would be 0.00741 X 20 = 0.1482ohms at 20 deg C.

The resistance of a conductor increases as it gets warmer, so we want to calculate the voltage drop at the maximum operating temperature of the conductor, when the resistance, and therefore voltage drop would be at its greatest. For T+E this is 70 deg C. A conductor at 70 deg C will have roughly 1.2 times the resistance of a conductor at 20 deg C.

So, 0.1482ohms X 1.2 = 0.17784ohms at 70 deg C.

V=IR
V = 13 X 0.17784
V = 2.31192V This is your voltage drop for the circuit.

Let's check that it tallies with the other method. From OSG P161:

1m 2.5mm² T+E has a VD of 0.018V/A/m. That's the VD for both line and neutral conductors, at 70 deg C.

0.018 X 13 X 10 = 2.34V/A/m

More or less the same, a very slight difference I expect due to rounding.

Note that I prefer to always work with volts rather than millivolts, which i think can confuse calculations sometimes.
So if the rn is not available the resistance and you have the r1 how do you find it or vice versa say you have to size of r1 but not rn say
 
So if the rn is not available the resistance and you have the r1 how do you find it or vice versa say you have to size of r1 but not rn say
So meaning when you go to look at the table for copper resistance and you have one but not the other how do you find it to complete resistance in calculation
 
So meaning when you go to look at the table for copper resistance and you have one but not the other how do you find it to complete resistance in calculation

For the example I gave, I used the data from the row saying "line conductor 2.5mm², protective conductor - ". This just gives you the resistance of 1m of a single 2.5mm² conductor. We were using 10m of twin and earth, which is 20m of conductor. Hence why I used 20m for the calculation.

Another way would be to use the data from the column "line conductor 2.5mm², protective conductor 2.5mm²" . This is the same as the resistance of 1m of 2 X 2.5mm² conductors in series, ie 1m of line conductor plus 1m of neutral conductor. Had I used this, I would have used 10m for the calculation instead.
 
So this would be as if both cpc and line conductors are the same Size but sometimes its not the case
CPC, line conductor, neutral conductor, it doesn't matter what they're called in the table. They're all copper, and they all have the same resistance per meter for a given cross sectional area. 1 meter of 2.5mm² twin and earth is 2 meters of live conductor: 1 meter of 2.5mm² line and 1 meter of 2.5mm² neutral.

Read back over my post carefully, it should explain things
 
To the OP: Focus on understanding the principle.. NOT a formula. The OSG & BS7671 & all the IET books that I've looked at... try to make things easier by giving you the same thing in a different way. But IMHO this just makes things far more confusing...

I think all the standard publications could be made half the size they are if they removed all the variations. Oh, and added page numbers to the index !!
 
To the OP: Focus on understanding the principle.. NOT a formula. The OSG & BS7671 & all the IET books that I've looked at... try to make things easier by giving you the same thing in a different way. But IMHO this just makes things far more confusing...
Completely agree with this. It's messy, and a nightmare when trying to learn. Eg the table on p196 should have just 3 columns: conductor CSA, resistance/m copper, resistance/m Aluminium. No need to mention line conductor, protective conductor, R1 or R2.
 
VD itself is as we know mV/A/m * Ib * L

Max VD is either 6.9v (3%) or 11.5v (5%) for lighting & power respectively

We can rearrange the formula (using Max & Actual VD) to find Max circuit length for the calculated VD



Let's say we have a 6 mm² T&E with pvc insulated and sheathed cable feeding a a lighting circuit which has a mV/A/m value of 7.3. The actual circuit current is 12.5 A, and the length of run is 14 m.
Volt drop = 7.3 x 12.5 x 14 / 1000
= 1.28 V


If a 14 m run gives a volt drop of 1.28 V,
the length of run for a 11.5 V drop will be:
11.5 x 14m = 105m
Completely agree with this. It's messy, and a nightmare when trying to learn. Eg the table on p196 should have just 3 columns: conductor CSA, resistance/m copper, resistance/m Aluminium. No need to mention line conductor, protective conductor, R1 or R2.
I'd drop the individual rows for line and CPC, as you say you just want a value for 2.5 and 1.5, doesn't matter if it's line neutral or CPC.

I disagree on dropping R1+R2, I find that useful for determining the length of a circuit (or an implausibly low/high reading), dividing my R1+R2 value by the listed value
 
I'd drop the individual rows for line and CPC, as you say you just want a value for 2.5 and 1.5, doesn't matter if it's line neutral or CPC.

I disagree on dropping R1+R2, I find that useful for determining the length of a circuit (or an implausibly low/high reading), dividing my R1+R2 value by the listed value
Problem is, you need both line and CPC columns present in order to have an R1+R2 column. Can't drop one without dropping the other!

Personally I think it clutters the mind when learning. And it's not difficult to calculate (R1+R2)/m if you have the resistance/m of each of the conductors: just add them together.

I would have the resistances in ohms/m as well. It would remove the annoying step of dividing by 1000 to convert from milli ohms to ohms.
 
The other basic method of working out the voltdrop they tend to use on the 2391 is using ohms law, I believe they use this to test the candidates basic knowledge

You would need to use your R1+RN mutipled by the design current and then mutilpying by 1.2 to allow for the circuit to be running at 70°c

A basic question would be
"Whats the volt drop on a 13 amp immersion circuit with an R1+RN of 0.30 ?"

A=4.68v
B=3.59v
C=4.45v
D=5.68v

Answer
13x0.3x(1.2) = 4.68v
 

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