Contents
The steady state behaviour of the rotating screen surrounding the inductor winding of the three-phase alternator with superconducting field winding is considered.
The armature positive and negative sequence magnetic fields, rotating with different velocities relative to the screen and present during steady state running due to unbalanced currents and armature reaction, are considered.
A calculation procedure to determine the radial and tangential components of the magnetic field in the screen, the current density and the power losses is described.
Through the calculation of the attenuation factor, the capacity of the screen to reduce the intensity of the magnetic field in the region occupied by the inductor winding is shown. Finally a numerical example is given.
Übersicht
Untersucht wird das stationäre Verhalten eines rotierenden Abschirmzylinders, der die supraleitende Erregerwicklung eines Drehstromgenerators umgibt. Betrachtet werden die mitlaufenden und inversen Drehfelder, die, durch Unsymmetrien hervorgerufen, relativ zum Abschirmzylinder mit verschiedenen Geschwindigkeiten umlaufen. Angegeben wird ein Rechenverfahren, mit dem das radiale und tangentiale magnetische Feld, die Stromdichte und Verluste im Abschirmzylinder bestimmt werden können. Durch Berechnung des Dämpfungsfaktors wird die Schirmwicklung auf den Raum erfaßt, in dem sich die Erregerwicklung befindet. Abschließend wird ein praktisches Beispiel durchgerechnet.
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Abbreviations
- ⋆:
-
vector Laplacian operator
- ★:
-
scalar Laplacian operator
- Re |.|:
-
real part of the argument in brackets
- Λ:
-
potential vector
- A* :
-
phasor notation of the potential vector when time-dependent
- a 1,a 2,b 1,b 2,c 1,c 2,d 1,d 2,e 1,e 2,f 2 :
-
real integration constants
- C :
-
attenuation factor
- E * :
-
phasor notation of imposed electric field
- G :
-
current density vector
- G * :
-
phasor notation of the current density vector when time dependent
- g, g′ :
-
real constants relating to the particular solution of the “Poisson-like” equation
- II :
-
magnetic field vector
- II * :
-
phasor notation of the magnetic field vector when timedependent
- H (1) :
-
Hankel function of the first kind
- h 1,h 2 :
-
real integration constants
- J :
-
Bessel function of the first kind
- K :
-
modified Bessel function of the second kind
- Ker, Kei:
-
real and imaginary parts ofK
- Ker′, Kei′:
-
first derivatives of Ker and Kei
- i, in :
-
complex constants
- M :
-
magnitude of the functionJ
- N :
-
magnitude of the functionK
- P :
-
power losses in the screen per unit length along the axis
- \(\dot p,\dot q,\dot s\) :
-
complex integration constants
- p, q :
-
magnitude ofp and\(\dot q\)
- r :
-
radial coordinate
- r 1,r 2,...,r 6 :
-
radii of the parts of the machine indicated in fig. 3
- t :
-
time variable
- \(\dot u\) :
-
complex variable
- v :
-
screen periferal velocity vector
- x :
-
\(\begin{array}{*{20}c} {\sqrt 2 } \\ {\delta ^v } \\\end{array}\)
- x 1 :
-
value ofx whenr=r 1
- x 2 :
-
value ofx whenr=r 2
- w :
-
real integration constant
- z :
-
axial coordinate
- α, β:
-
arguments of\(\dot p\) and\(\dot q\) respectively
- δ:
-
depth of current penetration in the screen
- η:
-
argument of the functionK
- ϑ:
-
angular coordinate
- μ:
-
absolute permeability
- μ0 :
-
vacuum permeability
- σ:
-
electrical conductivity of the screen
- φ:
-
angle of phase displacement
- ψ:
-
argument of the functionJ
- ω:
-
angular velocity, rotational speed
- 4:
-
number indicating the armature region
- i :
-
number indicating region of the machine (excluding the armature region)
- m :
-
rotor subscript
- n :
-
harmonic number, number of the order of Bessel function
- r :
-
radial subscript
- z :
-
axial subscript
- ϑ:
-
angular subscript
References
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This work has been carried out with the financial support of CNR
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Monti, C., Morini, A. & Verde, B. Steady state analysis of the magnetic fields and eddy currents in the rotating screen of a superconducting alternator. Archiv f. Elektrotechnik 57, 319–327 (1976). https://doi.org/10.1007/BF01575746
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DOI: https://doi.org/10.1007/BF01575746