application of a complex eigenmode solver to the tesla 1.3 ... 2013-08-09.… · august 19, 2013 |...
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Application of a Complex EigenmodeSolver to the TESLA 1.3 GHz Structure
W. Ackermann, C. Liu, W.F.O. Müller, T. WeilandInstitut für Theorie Elektromagnetischer Felder, Technische Universität Darmstadt
Status MeetingAugust 9, 2013DESY, Hamburg
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 1
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 2
Outline
Motivation
Computational model
- Problem formulation
- Planar ports of arbitrary shape
(here: coax lines and cylindrical beam tubes)
Numerical examples
- 1.3 GHz structure (single cavity)
Summary of all modes up to the 5th dipole passband
Summary / Outlook
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 3
Outline
Motivation
Computational model
- Problem formulation
- Planar ports of arbitrary shape
(here: coax lines and cylindrical beam tubes)
Numerical examples
- 1.3 GHz structure (single cavity)
Summary of all modes up to the 5th dipole passband
Summary / Outlook
19. August 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 4
Motivation
Linac: Cavities
- Photograph
- Numerical modelhttp://newsline.linearcollider.org
CST Studio Suite 2013
upstream downstream
Motivation
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 5
Superconducting resonator9-cell cavity
Downstreamhigher order mode coupler
Input coupler
Upstreamhigher order mode coupler
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 6
Outline
Motivation
Computational model
- Problem formulation
- Planar ports of arbitrary shape
(here: coax lines and cylindrical beam tubes)
Numerical examples
- 1.3 GHz structure (single cavity)
Summary of all modes up to the 5th dipole passband
Summary / Outlook
Computational Model
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 7
Geometrical model
9-cell cavity
Beamtube
DownstreamHOMcoupler
Input coupler
UpstreamHOMcoupler
High precision cavity simulations using FEM
on tetrahedral mesh
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 8
Computational Model
Port boundary condition
Port face, fundamental coupler
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 9
Computational Model
Port boundary condition
Port face, HOM coupler
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 10
Problem definition- Geometry
- Task
Numerical Examples
TESLA 9-cell cavity
PECboundary condition
Search for the field distribution, resonance frequency and quality factor
Portboundaryconditions
Port boundary conditions
Numerical Examples
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 11
Computational model
9-cell cavity
Beamcube
Inputcoupler
Upstream HOM coupler
Distributecomputational load
on multiple processes
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 12
Numerical Examples
Simulation results- Accelerating mode (monopole #9)
- Higher-order mode (dipole #37)
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 13
Numerical Examples
Simulation resultsAccelerating mode(monopole #9)
Higher-order mode(dipole #37)
Beam tube
HOM coupler
Coaxialinput coupler
Coaxial line
Beam tube
HOM coupler
Coaxialinput coupler
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 14
Outline
Motivation
Computational model
- Problem formulation
- Planar ports of arbitrary shape
(here: coax lines and cylindrical beam tubes)
Numerical examples
- 1.3 GHz structure (single cavity)
Summary of all modes up to the 5th dipole passband
Summary / Outlook
Numerical Examples
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 15
100
200
500100020005000
Monopole
Dipole
Quadrupole
Sextupole
2.46 2.48 2.50 2.52 2.54 2.56 2.58 2.600.00
0.01
0.02
0.03
0.04
Real
Imag
inar
y
Controlling the Jacobi-Davidson eigenvalue solver- Evaluation in the complex frequency plane- Select best suited eigenvalues in circular region around user-specified complex target
Real and imaginary part of the complex frequency
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 16
Numerical Examples
Quality factor versus frequency
Calculations kindly performed by Cong Liu
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 17
Numerical Examples
Simulation study based on mesh density variations- Grid 1
- Grid 2
- Grid 3
315.885 tetrahedrons1.932.746 complex DOF
1.008.189 tetrahedrons6.238.328 complex DOF
3.081.614 tetrahedrons19.177.820 complex DOF
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 18
Numerical Examples
Accuracy considerations (1st monopole passband)
Mod
e In
dex
Mod
e In
dex
Grid Index
Grid index:1) 315.885 tetrahedrons, 1.932.746 complex DOF2) 1.008.189 tetrahedrons, 6.238.328 complex DOF3) 3.081.614 tetrahedrons, 19.177.820 complex DOF
Relative error in ppmResonance frequency in GHz
Grid Index
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 19
Numerical Examples
Accuracy considerations (1st monopole passband)
Mod
e In
dex
Mod
e In
dex
Grid Index Grid Index
Grid index:1) 315.885 tetrahedrons, 1.932.746 complex DOF2) 1.008.189 tetrahedrons, 6.238.328 complex DOF3) 3.081.614 tetrahedrons, 19.177.820 complex DOF
Relative error in %Quality factor in 106
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 20
Numerical Examples
Accuracy considerations (1st monopole passband)
Mod
e In
dex
Mod
e In
dex
Grid Index
Grid index:1) 315.885 tetrahedrons, 1.932.746 complex DOF2) 1.008.189 tetrahedrons, 6.238.328 complex DOF3) 3.081.614 tetrahedrons, 19.177.820 complex DOF
Relative error in %Shunt impedance in MΩGrid Index
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 21
Numerical Examples
Collection of the first 194 modes (selected page)
Magnitude of the electric field strength(longitudinal cut)
Magnitude of the magnetic flux density(longitudinal cut)
Magnitude of the electric field and themagnetic flux density (longitudinal cut)
Resonance frequency, quality factorand shunt impedances
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 22
Numerical Examples
Comparison to MAFIA calculations (fres monopole)
Ref
eren
ce: (
TE
SLA
200
1-33
)M
onop
ole,
Dip
ole
and
Qua
drup
ole
Pas
sban
dsof
the
TE
SLA
9-c
ell C
avity
, R
. Wan
zenb
erg,
Sep
tem
ber
14, 2
001
Mod
e In
dex
Mod
e In
dex
TE modes
MAFIA:step size 1mm12.000 grid points
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 23
Numerical Examples
Comparison to MAFIA calculations (R/Q monopole)
Mod
e In
dex
Mod
e In
dex
TE modes
Ref
eren
ce: (
TE
SLA
200
1-33
)M
onop
ole,
Dip
ole
and
Qua
drup
ole
Pas
sban
dsof
the
TE
SLA
9-c
ell C
avity
, R
. Wan
zenb
erg,
Sep
tem
ber
14, 2
001
MAFIA:step size 1mm12.000 grid points
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 24
Numerical Examples
Geometry Modifications
CST cavity-construction macro:Modification of eachindividual cell possible
+ attachedbeam tubes and couplers
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 25
Numerical Examples
Geometry Modifications
Monopole #2
Monopole #9
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 26
Numerical Examples
Geometry Modifications
Monopole #2
Monopole #9
August 19, 2013 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Wolfgang Ackermann | 27
Summary / Outlook
Summary:Accurate complex eigenmode solver available
- FEM up to 2nd order edge elements
- Geometric modeling with curved tetrahedral elements
- Port boundary conditions with curved triangles
- Application to the 1.3 GHz structure(calculation of all modes up the 5th dipole passband)
Outlook:- Application to 1.3 GHz and 3.9 GHz cavity strings