Heat conduction in a cylinder crossed by an electric current with skin effect |
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Authors: | Antonio Barletta Enzo Zanchini |
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Institution: | (1) Istituto di Fisica Tecnica — Facoltà di Ingegneria, Università di Bologna, Viale Risorgimento, 2, I-40136 Bologna, Italy |
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Abstract: | The steady periodic temperature distribution in an infinitely long solid cylinder crossed by an alternating current is evaluated. First, the time dependent and non-uniform power generated per unit volume by Joule effect within the cylinder is determined. Then, the dimensionless temperature distribution is obtained by analytical methods in steady periodic regime. Dimensionless tables which yield the amplitude and the phase of temperature oscillations both on the axis and on the surface of copper or nichrome cylindrical electric resistors are presented.
Wärmeleitung in einem stromdurchflossenen Zylinder unter Berücksichtigung des Skin-Effektes Zusammenfassung Es wird die periodische Temperaturverteilung für den eingeschwungenen Zustand in einem unendlich langen, von Wechselstrom durchflossenen Vollzylinder ermittelt. Zuerst erfolgt die Bestimmung der zeitabhängigen, nichgleichförmigen Energiefreisetzung pro Volumeneinheit des Zylinders infolge Joulescher Wärmeentwicklung und anschließend die Ermittlung der quasistationären Temperaturverteilung auf analytischem Wege. Amplitude und Phasenverzögerung der Temperaturschwingungen werden für die Achse und die Oberfläche eines Kupfer- oder Nickelchromzylinders tabellarisch in dimensionsloser Form mitgeteilt. Nomenclature
A
integration constant introduced in Eq. (2)
- ber, bei
Thomson functions of order zero
-
Bi
Biot numberhr
0/
-
c
speed of light in empty space
-
c
1,c
2
integration constants introduced in Eq. (46)
-
c
p
specific heat at constant pressure
-
E
electric field
-
E
z
component ofE alongz
-
E
time independent part ofE, defined in Eq. (1)
-
f
function ofs and defined in Eq. (11)
-
g
function ofs and defined in Eq. (37)
-
h
convection heat transfer coefficient
-
H
magnetic field
-
i
imaginary uniti=(–1)1/2
-
I
electric current
-
I
eff
effective electric currentI
eff=I/21/2
- Im
imaginary part of a complex number
-
J
n
Bessel function of first kind and ordern
-
J
electric current density
-
q
g
power generated per unit volume
-
time average of the power generated per unit volume
-
time averaged power per unit length
-
r
radial coordinate
-
R
electric resistance per unit length
-
r
0
radius of the cylinder
- Re
real part of a complex number
-
s
dimensionless radial coordinates=r/r
0
-
s, s
integration variables
-
t
time
-
T
temperature
-
time averaged temperature
-
T
f
fluid temperature outside the boundary layer
-
time average of the surface temperature of the cylinder
-
u,
functions ofs, and defined in Eqs. (47) and (48)
-
W
Wronskian
-
x
position vector
-
x
real variable
-
Y
n
Bessel function of second kind and ordern
-
z
unit vector parallel to the axis of the cylinder
-
z
axial coordinate
- ·
modulus of a complex number
-
equal by definition
Greek symbols
amplitude of the dimensionless temperature oscillations
-
electric permittivity
-
dimensionless temperature defined in Eq. (16)
-
0,
1,
2
functions ofs defined in Eq. (22)
-
thermal conductivity
-
dimensionless parameter=(2)1/2
-
magnetic permeability
-
0
magnetic permeability of free space
-
function of defined in Eq. (59)
-
dimensionless parameter=c
p/()
-
mass density
-
electric conductivity
-
dimensionless time=t
-
phase of the dimensionless temperature oscillations
-
function ofs:=
1+i
2
-
angular frequency
-
dimensionless parameter=()1/2
r
0 |
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Keywords: | |
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