879

The resistance load line of a typical DC circuit can be analytically presented as:

where *Vs* stands for an open source voltage and *Rs* is system resistance including source and feeders. Introducing voltage drop across an arc *Varc*, arcing current can be expressed as:

where *Isc* is the available fault current at the point of arc and is equal to *Vs/Rs*. It was demonstrated that there is a minimum voltage needed to maintain an arc. That minimum depends on the current magnitude, gap width, and orientation of the electrodes. This transitional point can be expressed as:

where

*G* - conductor gap distance in millimeters

*It* - the transitional point current measured in amperes

Above that minimum, the arc V-I characteristic can be expressed as:

where

*Varc* - arcing voltage in volts

*Iarc* - dc arcing current in amperes

To find the point where the arc V-I characteristic crosses the circuit load line, solve equations (2) and (4) using the iterative method. As the first approximation, assume *Varc* is equal to half of the system voltage *Vs*. Then, follow the steps below:

- determine
*Iarc*from Equation (2) - substitute
*Iarc*into Equation (4) to determine new*Varc*

Cycle through the steps 1 and 2 above until the answers for *Varc* converge.

The energy released during an arc flash event is roughly proportional to the arc duration. The upstream protective device operation controls the arc flash duration. A fuse or properly maintained overcurrent protective device has a predictable time to open the circuit with a specific arc current value. Hence, arcing current impacts the released energy directly through the current itself and through interaction with the overcurrent protective device.

Additionally, circuit time constant affects current rise and protection device performance characteristics, thus impacting the arc duration. In this case, time current characteristic of the upstream protective device clearing the fault may have to be adjusted for the time constant. If this occurs, the process of determining the protective device operating time is cumbersome. First, the time-current characteristic of the protective device has to be analytically presented as a function of the available fault current. The relationship between the effective RMS current, the available fault current, and the number of time constants can be expressed as:

where the *K* factor is expressed in numbers of time constants *n = tarc/tconst*:

This creates a dilemma due to the fact that one cannot determine the arcing time without the RMS value of the arcing current, and one cannot solve for the RMS current without the arcing time represented by the *n* term in equation (6). This requires an iterative solution. As a first approximation, begin by assuming that *Irms* equals *Iarc*, determining *tarc* from the analytical expression for the protection device time-current characteristics *tarc=f(Irms)*, determining the number of time constants *n* and calculating *K* from equation (6), substituting its value into equation (5) to calculate the new RMS current, and then solving for the arc duration again. Once the first approximation of the arc duration has been made, determine the new number of time-constants *n*, re-calculate the *K* term and substitute its value into equation (5). This produces a new *Irms*. Re-calculate for a new *tarc* by using the new *Irms* and continue until the answers converge.

The power in the arc can be calculated by:

where the *Parc* is measured in watts.

The energy in the arc is a function of power and time:

where the *Earc* is measured in Joules.

Incident energy exposure for an open-air arc where the heat transfer depends on the spherical energy density is then expressed as:

where

*Eiair* - incident energy from an open air arc at distance *D* in Joules/cm^{2}

*D* - distance from the arc in centimeters

This formula assumes the radiant heat transfer. Not all of the arc energy will be transferred as radiant heat especially within the short time interval after the arc was ignited. Therefore, the equation (9) will produce a conservative but safe estimate of incident energy exposure.

For the arc in a box, the enclosure has a focusing effect on the incident energy. For the selected enclosure type and test distance, the incident energy from an arc flash in a box can be calculated by:

where

*Eibox* - the incident energy from an arc flash in a box in Joules/cm^{2}

*D* - distance from the arc in centimeters

*A* and *K* are obtained from optimal values listed in table below:

Enclosure Type | A, cm | K |
---|---|---|

Panelboard | 10 | 0.127 |

LV Switchgear | 40 | 0.312 |

MV Switchgear | 95 | 0.416 |

Equation (9) written in terms of arc flash boundary, becomes:

where

*AFB* - arc flash boundary is measured in centimeters

*Et* - threshold incident energy to second degree burn in J/cm^{2} calculated by:

Likewise, equation (10) written in terms of arc flash boundary, becomes:

© 2016 ARCAD INC. All rights reserved.