TY - BOOK
T1 - Dielectric window development for the ITER ICRF vacuum transmission line
AU - Heikinheimo, Liisa
AU - Heikkinen, Jukka
AU - Hytönen, Yrjö
AU - Linden, Juha
AU - Kemppainen, Markku
N1 - Project code: N6SU00180
PY - 1998
Y1 - 1998
N2 - The choice of dielectric material for the (double)
dielectric window of the ITER ICRF Transmission Line is
optimized with respect to nuclear, mechanical, and
thermal properties in due consideration of material
availability, fabrication issues and response to cyclic
loads. The window is optimized to minimize electric field
and thermal heating in the dielectric material with
specific cooling conditions and with constraints posed by
manufacturing. Electric field, temperature distribution,
and thermal stresses are evaluated for beryllia and
alumina dielectrics for unirradiated and irradiated
material data using IVOFEM/IVOHEAT and ANSYS finite
element code packages. The analysis is made for two
annular ceramic septa joined to inner (Ø 110mm) and outer
(Ø 196mm) coaxial water cooled conductors having maximum
operating 50kV peak RF voltage. Neutron radiation at the
window is evaluated from MCNP-4 calculations with account
for the neutron streaming through the structure of the
ICRF Array/Shield/VTL assembly. Placing beryllia windows
at the vacuum vessel feedthrough or outside is
acceptable, while alumina windows have to be positioned
outside the bio-shield unless additional shielding (30-60
cm thick) behind the ICRF array exists. For unfavourable
radiation conditions (5x10-2 dpa), alumina is found to be
heated excessively near 1000 oC with unacceptable
stresses. For beryllia (10-3 dpa) or for unirradiated
alumina (97.5 % purity), the temperature is found to stay
between the cooling temperature and 275 oC with maximum
principal stress less than 125 MPa, provided niobium,
titanium or materials with similar thermal expansion
coefficients are used as a conductor. Stresses with
steel, copper, or aluminium conductor are unacceptable.
Beryllia (BeO) is chosen as a candidate for the window
ceramic because of its better radiation resistance,
weaker temperature growth, and because of its better heat
conductivity helping the manufacturing process. The
dependence of the stress distribution on the material
data is presented including the additional impact from
the residual thermal stresses. The characteristics for
the ceramic/metal joints are estimated for candidate
conductor and ceramic materials. In particular, the
benefits from compatibility of thermal expansion in
ceramics and metal are investigated. Vacuum brazing using
active filler materials obviously provides sufficiently
good conditions for heat conduction, and appears to be
tight enough. The vacuum tightness, the strength against
the relative movements of the outer and inner conductors,
thermal expansion, and pressure shocks are investigated
with a full-scale preprototype experiment where two
alumina dielectrics (in an X-shaped geometry) are brazed
to a titanium coaxial housing and the tests shall be
performed for the system.
AB - The choice of dielectric material for the (double)
dielectric window of the ITER ICRF Transmission Line is
optimized with respect to nuclear, mechanical, and
thermal properties in due consideration of material
availability, fabrication issues and response to cyclic
loads. The window is optimized to minimize electric field
and thermal heating in the dielectric material with
specific cooling conditions and with constraints posed by
manufacturing. Electric field, temperature distribution,
and thermal stresses are evaluated for beryllia and
alumina dielectrics for unirradiated and irradiated
material data using IVOFEM/IVOHEAT and ANSYS finite
element code packages. The analysis is made for two
annular ceramic septa joined to inner (Ø 110mm) and outer
(Ø 196mm) coaxial water cooled conductors having maximum
operating 50kV peak RF voltage. Neutron radiation at the
window is evaluated from MCNP-4 calculations with account
for the neutron streaming through the structure of the
ICRF Array/Shield/VTL assembly. Placing beryllia windows
at the vacuum vessel feedthrough or outside is
acceptable, while alumina windows have to be positioned
outside the bio-shield unless additional shielding (30-60
cm thick) behind the ICRF array exists. For unfavourable
radiation conditions (5x10-2 dpa), alumina is found to be
heated excessively near 1000 oC with unacceptable
stresses. For beryllia (10-3 dpa) or for unirradiated
alumina (97.5 % purity), the temperature is found to stay
between the cooling temperature and 275 oC with maximum
principal stress less than 125 MPa, provided niobium,
titanium or materials with similar thermal expansion
coefficients are used as a conductor. Stresses with
steel, copper, or aluminium conductor are unacceptable.
Beryllia (BeO) is chosen as a candidate for the window
ceramic because of its better radiation resistance,
weaker temperature growth, and because of its better heat
conductivity helping the manufacturing process. The
dependence of the stress distribution on the material
data is presented including the additional impact from
the residual thermal stresses. The characteristics for
the ceramic/metal joints are estimated for candidate
conductor and ceramic materials. In particular, the
benefits from compatibility of thermal expansion in
ceramics and metal are investigated. Vacuum brazing using
active filler materials obviously provides sufficiently
good conditions for heat conduction, and appears to be
tight enough. The vacuum tightness, the strength against
the relative movements of the outer and inner conductors,
thermal expansion, and pressure shocks are investigated
with a full-scale preprototype experiment where two
alumina dielectrics (in an X-shaped geometry) are brazed
to a titanium coaxial housing and the tests shall be
performed for the system.
KW - fusion
KW - dielectric windows
KW - vacuum windows
KW - RF-heating
KW - dielectrics
M3 - Report
SN - 951-38-5254-7
T3 - VTT Publications
BT - Dielectric window development for the ITER ICRF vacuum transmission line
PB - VTT Technical Research Centre of Finland
CY - Espoo
ER -