Comparison of Poynting’s vector and the power flow used in electrical engineering
Source abstract
Abstract
This paper will analyze how the energy flux of Poynting’s vector is compared to the power flow in electrical engineering, where the power, instead, is defined by voltages and currents. There are alternatives to Poynting’s energy flux vector that agree more with circuit theory methods such that the energy flow is in the current conductor and not in the insulation surrounding it. One such basic formulation would only consist of the total current density and the voltage potential, but it would need an alternative theorem for energy transfer. Another formulation proposed by Slepian would instead still agree with Poynting’s energy transfer theorem, but it needs to add the power of alternating magnetic vector potential. The alternatives to Poynting’s vector may better illustrate the energy flow in electrical engineering, but two things could be considered in their generality. First, since they are expressed by potentials, they are gauge invariant and depend on the definition of the potentials. Second, Poynting’s vector is used to formulate the electromagnetic momentum, and any alternative energy flow vectors would not. These two notes are of minor importance in electrical engineering, and the alternatives could be used as good alternatives for describing power flow. The main purpose of this paper is to bridge the differences between the physical theory of energy flux and the methods in electrical power engineering. This could simplify the use of energy flux and Poynting’s vector in engineering problems.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Power Quality and Harmonics · Magnetic Properties and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Division of Electricity, Uppsala University , Uppsala 752 37, Sweden
References (71)
Show source-provided references
1. On the transfer of energy in the electromagnetic field10.1098/rstl.1884.0016 ↗
2. On the connexion between electric current and the electric and magnetic inductions in the surrounding field10.1098/rspl.1884.0080 ↗
3. On the connexion between electric current and the electric and magnetic inductions in the surrounding field10.1098/rstl.1885.0003 ↗
4. Energy flow in electric systems-the Vi energy-flow postulate10.1109/t-aiee.1942.5058450 ↗
5. Energy and energy flow in the electromagnetic field10.1063/1.1714903 ↗
6. Application of the Poynting vector for power conditioning and conversion10.1109/13.9751 ↗
7. Energy transfer in electrical circuits: A qualitative account10.1119/1.1819932 ↗
8. Energy flow from a battery to other circuit elements: Role of surface charges10.1119/1.3456567 ↗
9. Where is the Poynting vector in an ideal transformer?10.1119/1.13563 ↗
10. The Poynting vector in a transformer10.1119/1.13912 ↗
11. The Poynting vector field and the energy flow within a transformer10.1119/1.14554 ↗
12. The Poynting vector distribution in a simple transformer10.1119/1.15134 ↗
13. Flow of energy in D-C machines10.1109/tce.1953.6372029 ↗
14. Flow of energy in synchronous machines10.1109/tce.1954.6372102 ↗
15. Étude d’une machine à induction par la méthode du vecteur de Poynting
16. The flow of electric power in electrical machines
17. Le théorème de Poynting en électrotechnique
18. 1950 · 1
19. Poynting vector analysis of synchronous generators using field simulations10.1109/tmag.2007.893166 ↗
20. Air-gap power flow and torque development in electrical machines-can we teach the fundamentals?10.1109/tpas.1984.318366 ↗
21. Poynting theorem applied to cable wound generators10.1109/tdei.2008.4483482 ↗
22. On the flux of energy in the electrodynamic field10.1080/14786441108635713 ↗
23. 1926
24. Alternative choice for the energy flow vector of the electromagnetic field10.1119/1.12719 ↗
25. 1902
26. Electromagnetic energy density and flux10.1139/p52-013 ↗
27. Energy flow vector of the electromagnetic field10.1139/p80-101 ↗
28. Alternatives to the Poynting vector for describing the flow of electromagnetic energy10.1119/1.12903 ↗
29. Poynting in the wrong direction?10.1088/0143-0807/3/2/005 ↗
30. A note on the uniqueness of the Poynting vector and of the Maxwell tensor10.1002/jnm.2214 ↗
31. 1999
32. 1989
33. 1999
34. The Poynting vector and power in a simple circuit10.1119/1.1302733 ↗
35. Visualizing Poynting vector energy flow in electric circuits10.1119/1.3679838 ↗
36. Poynting vector flow in a circular circuit10.1119/1.3630927 ↗
37. Demonstration of the electric fields of current-carrying conductors10.1119/1.1941887 ↗
38. 1964
39. On the forces, stresses, and fluxes of energy in the electromagnetic field10.1098/rsta.1892.0011 ↗
40. VIII. A dynamical theory of the electromagnetic field10.1098/rstl.1865.0008 ↗
41. Powers in nonsinusoidal situations-a review of definitions and physical meaning10.1109/61.57980 ↗
42. On the definition of power in an electrical system10.1109/tpwrd.2007.893194 ↗
43. A review and insights on Poynting vector theory and periodic averaged electric energy transport theories10.1016/j.rser.2014.10.065 ↗
44. Could power properties of three-phase systems be described in terms of the Poynting vector?10.1109/tpwrd.2005.852353 ↗
45. 2002
46. 1894 · 93
47. 1893 · 313
48. Physical significance of the Poynting vector in static fields10.1119/1.1973915 ↗
49. 1967 · 318
50. Energy flux vector for the electromagnetic field and gauge invariance10.1119/1.12901 ↗
51. Objections to an alternate energy flow vector10.1119/1.13024 ↗
52. On the uniqueness of the vector for energy flow density in electromagnetic fields10.1119/1.14646 ↗
53. From Lorenz to Coulomb and other explicit gauge transformations10.1119/1.1491265 ↗
54. Alternative choice for the energy flow vector of the electromagnetic field10.1119/1.12795 ↗
55. Introducing electromagnetic field momentum10.1088/0143-0807/33/4/873 ↗
56. Linear momentum of quasistatic electromagnetic fields10.1119/1.1972282 ↗
57. Linear momentum of the source of a static electromagnetic field10.1119/1.1986204 ↗
58. An exact formula for electromagnetic momentum in terms of the charge density and the Coulomb gauge vector potential10.1088/1361-6404/aa9051 ↗
59. Electromagnetic momentum density and the Poynting vector in static fields10.1119/1.17738 ↗
60. ‘Try simplest cases’ discovery of ‘hidden momentum’ forces on ‘magnetic currents’10.1103/physrevlett.18.876 ↗
61. Origin of ‘hidden momentum forces’ on magnets10.1103/physrev.171.1370 ↗
62. Examples of momentum distributions in the electromagnetic field and in matter10.1119/1.1975729 ↗
63. Concerning ‘hidden momentum’10.1119/1.2815366 ↗
64. Hidden momentum, field momentum, and electromagnetic impulse10.1119/1.3152712 ↗
65. Mansuripur’s paradox10.1119/1.4812445 ↗
66. Angular momentum of static electromagnetic fields10.1119/1.1973478 ↗
67. Feynman’s disk paradox10.1119/1.13272 ↗
68. Field angular momentum in Feynman’s disk paradox10.1119/1.14801 ↗
69. Elementary solution to Feynman’s disk paradox10.1119/1.14387 ↗
70. More on the Feynman’s disk paradox10.1119/1.13853 ↗
71. Letter to the editor10.1119/1.13214 ↗