the design of elliptical cavities
DESCRIPTION
The design of elliptical cavities. Gabriele Costanza. Introduction. To design a cavity we need to characterize it from an electromagnetic and mechanical point of view. Manufacturing , cleaning , testing - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/1.jpg)
The design of elliptical cavities
Gabriele Costanza
![Page 2: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/2.jpg)
Introduction
• Design = optimization of the shape of the cavity with respect to a set of parameters– RF parameters– Mechanical parameters
• Manufacturing, cleaning, testing– Chemical polishing: Buffered Chemical
Polishing or Electrop-polishing. Removes a damaged surface layer (due to the manufacturing process) and reduces roughness.
– Heat treatment: removes H from the – Rinsing with high pressure, ultrapure water
• To design a cavity we need to characterize it from an electromagnetic and mechanical point of view
![Page 3: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/3.jpg)
Introduction• The medium β cavity has
5 cells and operates in the TM01π mode.
• The longitudinal E-field has a 180 phase shift from one cell to the next so that the particles experience always an accelerating field. The length of each cell is then:
![Page 4: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/4.jpg)
IntroductionMulticell structures:• Less expensive/m !!• Fewer couplers, easier phasing…..
Advantages of single cell structures:• No field flattness problem• Easier to damp HOMS• The input coupler transfers less
power• Easier to manufacture and clean
![Page 5: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/5.jpg)
Example: pillbox • The simplest model of an accelerating cavity = pillbox• Let’s consider a pillbox of radius a and length h.• To find the fields of the accelerating mode (TM010) we need to solve the transverse
problem:• • and the longitudinal problem:
• The solution consists in the eigenmodes and eigenvalues.• The accelerating (fundamental) mode is the (TM010):
• The dispersion relation is:
• For the TM010 mode to resonate at 704.42 MHz, a=16.29 cm
![Page 6: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/6.jpg)
RF parameters
THE DESIGN OF ELLIPTICAL CAVITIES
![Page 7: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/7.jpg)
RF parameters• With the fields we can calculate
several quantities:• Stored Energy:
• Power Dissipated:– part of the energy stored in the
cavity is dissipated on the walls
• Power exchanged with the external circuit:
– Power extracted by the HOM coupler or injected by the FPC
port
![Page 8: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/8.jpg)
RF parameters• Intrinsic quality factor Q0: • Measures of how quickly the energy stored in the cavity is lost by dissipation in the cavity
walls. • External quality factor Qext: • Measures how quickly the energy stored in the cavity is radiated through the ports .• Geometric factor: • Measures of the energy lost by dissipation in the cavity walls considering a Rsurf of 1 ohm. • The surface resistance of SC structures can be modeled with:
• The residual resistance is almost constant with temperature and is a measure of the quality of the material. The clearner the surface, and the purer the metal, the lower is the residual resistance.
• The BCS resitance grows very quickly with the frequency and decreases exponentially with the temperature.
![Page 9: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/9.jpg)
RF parameters• We define the R/Q as:
• Where:
is a measure of how efficient the cavity accelerates the beam, • a large R/Q implies that little energy is required to
produce a large acceleration, therefore the R/Q is a measure on how efficient the energy exchange between a mode and the beam is (beam coupling impedance)
• R/Q does not depend on the material of the cavity.
![Page 10: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/10.jpg)
RF parameters• The higher the parameter: the higher the accelerating voltage with respect to the power dissipated• Peak Fields:– Epk/Eacc , where Epk is the peak electric
field on the surface of the cavity and – Bpk/Eacc [mT/(MV/m)] , where Bpk is the
peak magnetic field on the surface of the cavity.
![Page 11: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/11.jpg)
RF parameters• Cell to Cell Coupling Kcc: • It’s a measure of the width of a
band. It’s usually calculated only for the fundamental passband.
• It’s important to have a high cell-to-cell coupling because:– It’s easier to obtain a high field
flattness, that is, field is more even among cells
– enhanced frequency separation between the 4π/5 and the π modes
– HOMs are better coupled to the outer cells and possibly extracted by an antenna
![Page 12: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/12.jpg)
RF parameters: summary• Rf parameters summary:
,these are not the only parameters to take into account…
• The end cells and the inner cells are different because the outer cells are connected to the beam tubes, so I consider them separately
• Let’s take a look at geometry of the inner cell:– 6 geometric parameters:
• A,B = radiuses of the major ellipse• a,b = radiuses of the smaller ellipse• Riris = the radius of the iris• D = the diameter of the cell is a tuning
parameter• The end cells add other 5 parameters (for
symmetric cavities)
![Page 13: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/13.jpg)
Mechanical parameters
THE DESIGN OF ELLIPTICAL CAVITIES
![Page 14: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/14.jpg)
Mechanical parameters• Assume a wall thickness of 3.6 mm• Cavity Stiffness [KN/mm]: 1 KN is applied at one end, the other end is
grounded. The displacement is calculated
• Tuning Sensitivity Δf/Δz [KHz/mm]: a displacement of 1 mm is imposed at one end, the other end is grounded. The new frequency of the π mode is calculated.
1 KN
![Page 15: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/15.jpg)
Mechanical parameters• Pressure Sensitivity [Hz/mbar]: vibrations coming from various sources
cause the detuning of the cavity. The major contributor is the variation of the helium pressure. In this simulation a uniform pressure of 1 mbar is applied to the external boundary. The frequency shift is calculated. Both ends are grounded
![Page 16: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/16.jpg)
Mechanical parameters• Lorentz Detuning Coefficient [Hz/(MV/m) 2]: The Lorentz Detuning Coefficient is defined as
• The frequency detuning is caused by the EM pressure on the cavity walls. The pressure is
• Both ends are grounded
![Page 17: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/17.jpg)
Design
THE DESIGN OF ELLIPTICAL CAVITIES
![Page 18: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/18.jpg)
Design • The radius of the iris is a very powerful variable to trim the RF parameters• All the other parameters have a ”second order” influcence• Too many parameters to design an entire cavity all at once• Design flow:
• All the cells are designed with COMSOL. I wrote a code to explore one section of the parameter space at a time. The code launches COMSOL to simulate the structure, tunes the cell to 704 MHz and calculates the RF parameters. The mechanical simulations are performed only on the full cavity.
• There are 5 RF parameters, the optimal choice is not obvious! (tradeoffs)
Inner cell
RF Parameter calculation & selection of the best geometry
end cell
RF Parameter calculation & selection of the best geometry
cavity
![Page 19: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/19.jpg)
Parameter trends• All the parmeters are connected between each other and it’s not clear what
the ”best solution” is• For example:
Riris
KccPeak Fields
R/QG
![Page 20: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/20.jpg)
parameter increases
Bpk/Eacc Epk/Eacc
A - ~+
B ~ ~
a ~ ~-
b ~- -
More on parameter trends
- A ”tall” minor ellipse leads to a lower electric peak field (α increases).- A ”large” major ellipse leads to a lower magnetic peak field- B has little influence on the RF properties.- The same applies to the outer cells but it’s harder to achieve the same performance due to the beam tube
High peak fields can limit the maximum achievable gradient
![Page 21: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/21.jpg)
The code• The optimizing code…
![Page 22: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/22.jpg)
The code• The optimizing code…
![Page 23: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/23.jpg)
Results
THE DESIGN OF ELLIPTICAL CAVITIES
![Page 24: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/24.jpg)
RF parametersR/Q[Ohm] 302.30 308.29 309.81
G[Ohm] 198.7 204.5 203.58
G R/Q [Ohm2] 60077 63069 63071
Epk/Eacc 2.508 2.6052 2.5578
Bpk/Eacc [mT/MV/m] 4.936 4.8097 4.816
Field flattness [%] 99.98 99.967 99.93
Kcc [%] 1.32 1.43 1.36
Freq. distance between 4π/5 and π mode [KHz]
840 908.7 861.8
Mechanical parameters (no stiffening rings)Cavity Stiffness [KN/mm]
0.956 0.714 0.659
Tuning Sensitivity Δf/Δz [KHz/mm]
244.9 239.4 244.2
KL [Hz/(MV/m) 2]Both ends fixed
1.739 1.499 1.53
Pressure Sensitivity [Hz/mbar]
28.7 35.6 34
63+2 57_2+20 63_2+31Found in ”Medium β Elliptical Cavity – Cyromodule Technology Demonstrator”. S. Molloy
Epk/Eacc < 2.63 Epk/Eacc < 2.66
Bpk/Eacc< 5.26 mT/MV/m
Bpk/Eacc < 5.33 mT/MV/m
Can we use higher gradients?
larger dome ellipse=>higher Kcc
![Page 25: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/25.jpg)
ResultsCourtesy of Paolo Pierini, HPSL Workshop
SPL CDR II
4.5 cm Riris to increase The R/Q but a lower beta Leads to higher Kcc
Lower beta => lower R/Q=> Smaller Riris
![Page 26: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/26.jpg)
Results63+2
![Page 27: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/27.jpg)
Results63+2
![Page 28: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/28.jpg)
Results63+2
• The cavities tend to have better performances for β> βg
![Page 29: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/29.jpg)
Results63+2
![Page 30: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/30.jpg)
Results
The cavities must be tuned to obtain a high field flattness
![Page 31: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/31.jpg)
Results63+2
![Page 32: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/32.jpg)
Results57_2+20
![Page 33: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/33.jpg)
Results57_2+20
![Page 34: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/34.jpg)
Results57_2+20
![Page 35: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/35.jpg)
Results
![Page 36: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/36.jpg)
Results57_2+20
![Page 37: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/37.jpg)
Results63_2+31
![Page 38: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/38.jpg)
Results63_2+31
![Page 39: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/39.jpg)
Results63_2+31
![Page 40: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/40.jpg)
Results63_2+31
![Page 41: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/41.jpg)
Results63_2+31
![Page 42: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/42.jpg)
Bonus Section (if you’re not too bored….)
THE DESIGN OF ELLIPTICAL CAVITIES
SLUT, TACK
![Page 43: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/43.jpg)
Results: HOM 1pole list
All HOMs with their R/Q’s are calculated up to 3 GHz.Study of the HOMs started
Two modes close to 6f0 :f0 = 352.21 MHz
2.111337 GHz
2.11135 GHz
Does this mode really exist?
![Page 44: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/44.jpg)
On the number of cells per cavity
1. The lowe the number of cells, the higher the maximum Eacc. The maximum is not obtained at the geometric beta
2. The higher the number of cells, the lower the energy / velocity acceptance but 4 cell cavities lead to longer accelerator & more €
βg
![Page 45: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/45.jpg)
On the number of cells per cavity
Cryostat Filling Factor = Cryostat accelerating efficiency
=
4 cavities per cryo5 cavities per cryo
6 cavities per cryo
βg =0.65
βg =0.67
βg =0.69
1 m
15 cm
10 cm
2 m
Is a higher βg better?
![Page 46: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/46.jpg)
On the number of cells per cavity
• Higher βg => wider energy/velocity acceptance, higher injection energy => more spokes. Are they more efficient / less expensive than elliptical cavities?
• If not it’s possible to use ”few” βg = 0.65 ell. cavities (lower injection energy) and more high β cavities which are more efficient than βg = 0.67 cavities
• Lower βg => lower performances (but it’s possible to find a good compromise). Cavities for βg <1 have a smaller volume, for the same frequency, w.r.t βg =1 cavities, and lower Eacc because of the reduced length => higher peak fields
βg
![Page 47: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/47.jpg)
![Page 48: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/48.jpg)
RF parametersR/Q[Ohm] 309.81
G[Ohm] 203.58
G R/Q [Ohm2] 63071
Epk/Eacc 2.5578
Bpk/Eacc [mT/MV/m] 4.816
Field flattness [%] 99.93
Kcc [%] 1.36
Freq. distance between 4π/5 and π mode [KHz]
861.8
Mechanical parameters (w stiffening rings)Cavity Stiffness [KN/mm] 1.65
Tuning Sensitivity Δf/Δz [KHz/mm]
254.4
KL [Hz/(MV/m) 2]Both ends fixed
0.93
Pressure Sensitivity [Hz/mbar]
0.67
63_2+31
Simulations of stiffened cavities
![Page 49: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/49.jpg)
RF parameters
R/Q[Ohm] 302.304 64.6715 59.7
G[Ohm] 198.7338 196.637 201.87
Epk/Eacc 2.508 2.452 2.4725
Bpk/Eacc [mT/MV/m] 4.936 4.8389 4.8646
Field flattness [%] 99.98
Kcc [%] 1.32 1.302
Freq. distance between 4π/5 and π mode [ KHz]
840
Mechanical parameters
Cavity Stiffness [KN/mm] 0.956
Tuning Sensitivity Δf/Δz [KHz/mm]
244.5
KL [Hz/(MV/m) 2]Both ends fixed
1.739
Pressure Sensitivity [Hz/mbar]
28.68
63+2 63 2
Some results
![Page 50: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/50.jpg)
RF parameters
R/Q[Ohm] 308.29 66.2645 60.625
G[Ohm] 204.5778 202.92 207.05
Epk/Eacc 2.6052 2.5284 2.5546
Bpk/Eacc [mT/MV/m] 4.8097 4.6875 4.7496
Field flattness [%] 99.967
Kcc [%] 1.43 1.4
Freq. distance between 4π/5 and π mode [ KHz]
908.7
Mechanical parameters
Cavity Stiffness [KN/mm] 0.714
Tuning Sensitivity Δf/Δz [KHz/mm]
239.4
KL [Hz/(MV/m) 2]Both ends fixed
1.499
Pressure Sensitivity [Hz/mbar]
84
57_2+20 57_2 20Some results
![Page 51: The design of elliptical cavities](https://reader035.vdocuments.mx/reader035/viewer/2022062305/5681625c550346895dd2b32f/html5/thumbnails/51.jpg)
RF parameters
R/Q[Ohm] 309.81 66.59 60.91
G[Ohm] 203.58 201.69 206.39
Epk/Eacc 2.5578 2.4996 2.5192
Bpk/Eacc [mT/MV/m] 4.816 4.6991 4.7511
Field flattness [%] 99.93
Kcc [%] 1.36 1.339
Freq. distance between 4π/5 and π mode [ KHz]
861.8
Mechanical parameters
Cavity Stiffness [KN/mm] 0.659
Tuning Sensitivity Δf/Δz [KHz/mm]
244
KL [Hz/(MV/m) 2]Both ends fixed
1.5
Pressure Sensitivity [Hz/mbar]
43
63_2+31 63_2 31
Some results