An Electical Arc-Flash Hazard Analysis Primer: Reducing Arc-Flash Hazard Exposures Through Engineering Controls

Author(s):  
John J. Kolak

The problem of electrical workers being injured or killed by electrical arcs and blasts is one of the most significant safety issues in the industry today. Accident data reveals that over 2,000 people are severely burned annually by electrical arc blasts on the job (1) and many others receive less severe burns that still result in significant pain and suffering to the victim. The purpose of this presentation is to provide an overview of the arc-flash hazard analysis (AFHA) process and general guidance for those organizations wishing to integrate AFHA into their overall electrical safety program. The electric utility industry was the first non-academic group to study arc-flash hazards (AFH) when they noted that electrical workers often received the most severe burns from their clothing igniting and continuing to burn long after the initiating arc had extinguished. In particular, man-made fibers such as polyester, nylon, and rayon were known to melt and stick to the worker’s skin following an AF, and this resulted in burns many times worse than had the injured worker been wearing no clothing at all (2). Subsequent studies were performed by private organizations and they impacted both the engineering and safe work practices associated with industrial plant operations. The primary standards or studies included: • IEEE 1584 Guide for Performing Arc-Flash Hazard Calculations • NFPA 70E Standard for Electrical Safety in the Workplace • OSHA 29 CFR 1910.269: Electrical Power Generation, Transmission, and Distribution Standard Of these documents, the IEEE 1584 Guide was most influential to engineers because it provided formulas for calculating incident energy levels, arc-flash protection boundaries, and a host of other important variables necessary to evaluate AFH in the work place. The term ‘incident energy’ refers to the amount of heat concentrated per unit-area of the skin. Incident energy is measured in calories per square centimeter (cal/cm2) of skin surface area. For reference, a value of 1.2 cal/cm2 will result in a second-degree burn of human skin (3). The principal reason why AFHA is necessary is that studies revealed that electrical arcs are somewhat unpredictable events (4), and there were many cases where seemingly innocuous energy sources (small transformers) produced incident energy levels that far exceeded the limitations of flame resistant (FR) clothing or other forms of personal protective equipment. It became obvious that the best method for protecting employees from AFH would be to evaluate the hazard level and then mitigate it through the use of engineering controls. Paper published with permission.


2021 ◽  
Author(s):  
MARINA CAMPONOGARA ◽  
ANA PAULA GHESTI MARCHESAN ◽  
DANIEL PINHEIRO BERNARDON ◽  
RAFAEL GRESSLER MILBRADT ◽  
TIAGO BANDEIRA MARCHESAN ◽  
...  

The thermal hazard is considered the most significant hazard from an arc flash event. The protection against this type of hazard is associated with the assessment of incident energy, a study that aims to analyze the possibility of occurrence of an electric arc, the incident energy produced by it and the necessary protections so that the work in electricity is safe. An incident energy analysis is performed to the 634 bus of IEEE 13 Node system using the ATP Draw software to simulate a three-phase shot-circuit and an online platform that runs the IEEE Std 1584-2018 model is employed to obtain the incident energy levels and arc-flash boundary values for different durations of arcing event. As a closing, the personal protective equipment required for the different time scenarios are analyzed, according to the two approaches proposed in NFPA 70E-2021.



2021 ◽  
Author(s):  
Abdeslem Kadri

Arc flashes in power system result in a huge amount of incident energy that can injure human workers. Strict safety measures have to be applied in the work place for safety of technical personnel. Computation of the incident energy is imperative to determine the corresponding safety requirements. Arcing current, and hence incident energy, is a function of some system parameters which may vary due to different reasons. This research work considers the problem of parameter variability in arc flash calculations and its effect on hazard mitigation. A mathematical basis is set forth for the impact of the variation in gap between electrodes and system voltage on the incident energy value. Findings of this work emphasize that small variations in system parameters can yield inaccurate values of incident energy and misleading hazard categories. Therefore, parameter variation has to be carefully accommodated in the arc flash calculations to result in the proper hazard mitigation precautions.



2021 ◽  
Author(s):  
Abdeslem Kadri

Arc flashes in power system result in a huge amount of incident energy that can injure human workers. Strict safety measures have to be applied in the work place for safety of technical personnel. Computation of the incident energy is imperative to determine the corresponding safety requirements. Arcing current, and hence incident energy, is a function of some system parameters which may vary due to different reasons. This research work considers the problem of parameter variability in arc flash calculations and its effect on hazard mitigation. A mathematical basis is set forth for the impact of the variation in gap between electrodes and system voltage on the incident energy value. Findings of this work emphasize that small variations in system parameters can yield inaccurate values of incident energy and misleading hazard categories. Therefore, parameter variation has to be carefully accommodated in the arc flash calculations to result in the proper hazard mitigation precautions.



Author(s):  
Saad. M. Saad ◽  
Naser El Naily ◽  
Abdelsalam Elhaffar ◽  
T. Hussein ◽  
Faisal A. Mohamed


2020 ◽  
Author(s):  
J.C. Das
Keyword(s):  


The study of collisions between nuclear particles has developed to a remarkable extent with the discovery of the neutron and the introduction of artificial methods for effecting nuclear disintegration. It has been found in the last few years that the interpretation of the observed results is by no means as simple as was first expected. This situation is most apparent when the explanation of the variation of probability of capture of slow neutrons by different nuclei is considered. This probability varies in a very irregular manner from element to element and pronounced selective effects occur in certain cases. Attempts to explain (Elsasser and Perrin 1935; Bethe 1935) these resonance phenomena in terms of the usual approximations of quantum collision theory were soon found to be inadequate, All such attempts were based on the assumption that the Chance of a nuclear collision being elastic is high compared with that of its resulting in capture or excitation. A high probability of capture (with emission of radiation) or excitation could then only appear together with a high probability of elastic collision and this is frequently contradicted by the experimental results. The sharpness of the observed resonance phenomena was also difficult to under­stand on this basis. It was first pointed out by Bohr (1936) that the initial assumptions concerning the probability of elastic collisions, virtually involving the treatment of the elastic scattering as a one-body problem in the first approximation, cannot be valid for nuclei in which the particles, even is existing separately in the nuclei at all, are so closely packed. On making a close collision with a nucleus a particle, such as an α -particle, neutron or proton, comes into close and strong interaction with a number of nuclear particles and its incident energy becomes distributed among them. It is only when a particular particle receives sufficient energy to leave the quasi-stable complex formed that a disintegration particle is emitted. (This may of course be the original incident particle, in which case the collision would be an elastic or excitation one.) Otherwise the surplus energy is emitted as radiation. The resonance phenomena arise from the energy levels of the quasi-stable complex. If the incident energy is such that the total energy is equal or nearly equal to that of one of these energy levels, the range of interaction and hence the collision cross-section is quite large. This point of view must be adopted not only when dealing with neutron collisions but in all cases in which the impinging particle does not possess an energy greatly in excess of the minimum necessary for the process to occur. Disintegrations produced by charged particles, in which resonance effects have been observed for some time (Feather 1937, P. 154), must therefore be capable of description in this way.



2014 ◽  
Vol 20 (4) ◽  
pp. 6-6
Author(s):  
Ben C. Johnson ◽  
Mary Capelli-Schellpfeffer


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