HiRadMat Window Design report v3.0 Michael MONTEIL - 12 April 2010 1 Specifications v3.0 • Interface between machine vacuum and Atmospheric pressure 10-8 mbar / Patm Protective atmosphere !!! • Aperture min 60 mm • Resist to a proton beam size on the window : 1s = 0.5 mm “Beam Size at the TT66 Vacuum Window”, C. Hessler, 26.02.2010 Michael MONTEIL - 12 April 2010 2 Solution #5 : Be + C-C • Same as solution #4 but the pressure load is supported by a C-C plate ⁺ ⁺ ⁺ ⁺ Simple window assembly Thin thickness (no differential pumping…) Be cannot pollute vacuum chamber unless C-C fail Tight ⁻ Price of Be but no pumps Michael MONTEIL - 12 April 2010 3 Solutions - Sum-up • #1: C-C (Differential pumping) – Protective atm (Nitrogen ?) – Radiations? • #2: C-C + Graphite foil (useless now) • #3: Tight steel “ring” with a C-C plate • #4: Beryllium – Safety problem • #5: C-C + Beryllium Today Michael MONTEIL - 12 April 2010 4 Different grades of Be Michael MONTEIL - 12 April 2010 Data: Brush Wellman 5 Different grades of Be • PF-60 ? – Low rate of Beryllium oxide compare to PS-200 – Good quality-price ratio (Next slides…) • 1.5 to 2 time cheaper than IF-1 – Almost the same temperature distribution as pure Be and IF-1 (IF-1 a bit better…) – Used in CNGS… Michael MONTEIL - 12 April 2010 Collaboration: J. Blanco 6 Design • Specification – Be & C-C – Aperture min. 60mm – DN80 or DN60 conical flange connection – 15 cm depth maximum • Remark – Cannot machine Be at CERN Michael MONTEIL - 12 April 2010 7 Design • Common design – Choices – Standard flanges only (cheaper) – Be window assembled in lab between 2 flanges (safety) – Conical flange (faster assembly once in experimental area) Design Conical Flange (plug-in flange) Tube (connection conical flange <--> conflat flange) 2 x Conflat (Window in-between) Michael MONTEIL - 12 April 2010 8 “CNGS” like CNGS HiRadMat – Option 1 Nota: Those drawing are drafts. Above dimensions are not representative of the reality Michael MONTEIL - 12 April 2010 9 “CNGS” like Data: Brush Wellman Michael MONTEIL - 12 April 2010 10 “CNGS” like Data: Brush Wellman Michael MONTEIL - 12 April 2010 11 “TED @ TI2, TT40” – Beryllium version “TED @ TI2, TT40” HiRadMat – Option 2 Michael MONTEIL - 12 April 2010 12 “TED @ TI2, TT40” – Beryllium version • Quote from BW Michael MONTEIL - 12 April 2010 13 2 design proposals Option 1 Option 2 + Life warranty on Be + flange assembly + Easy to assembly + Standard conflat assembly + Tightness OK - Not that much + Not that much - Precautions for the assembly - Non Standard conflat assembly (Tightness) - Might be careful to not cut (shear cut) the Be foil during assembly Nota: Those drawing are drafts. Above dimensions are not representative of the reality Michael MONTEIL - 12 April 2010 14 2 design proposals Cost estimation Be Foil Option 2 Option 1 • Number of flange to order : 2 • Number of foil to order : 3 – Spare : 1 – Window installed : 1 – Spare : 1 – Window installed : 1 – “In case we break a foil while assembling” : 1 Nota: Those drawing are drafts. Above dimensions are not representative of the reality Michael MONTEIL - 12 April 2010 15 2 design proposals Cost estimation Be Foil Option 1 Flange Grade IF-1 Quantity 1 2 3 4 5 Foil 0.254 mm 6384 2128 8228 2057 10220 2044 0.254 mm 2552 2552 5104 2552 7656 2552 10208 2552 12760 2552 Flange 0.381 mm 3266 3266 6532 3266 9798 3266 13064 3266 16330 3266 Grade PF-60 Quantity 1 2 3 Foil 0.254 mm 3192 1064 0.254 mm 1944 1944 3888 1944 5832 1944 Flange 0.381 mm 1903 1903 3806 1903 5709 1903 4 3968 992 7776 1944 7612 1903 Option 2 Foil 5 4895 979 9720 1944 9515 1903 Grade PS-200 Quantity 1 2 3 4 5 Foil 0.254 mm 0.254 mm 1890 1890 3780 1890 5670 1890 7560 1890 9450 1890 Flange 0.381 mm 1866 1866 3732 1866 5598 1866 7464 1866 9330 1866 Nota: Those drawing are drafts. Above dimensions are not representative of the reality Michael MONTEIL - 12 April 2010 16 About thickness, how does BW design their own Be foils? Data: Brush Wellman With (Thickness 0.25mm, radius 35mm, pressure 1.01 kPa, E 303Gpa, Poisson 0.08) Results – – sedge= 305MPa > 275 Mpa !! scenter= 297Mpa > 275 Mpa !! Michael MONTEIL - 12 April 2010 17 However… • BW : “With confirm that your calculations with reference to the DB450277 assembly are correct and show over the recommended values, however, the assembly was designed using empirical data as well taking into consideration the calculated values. We have performed tests on this design and found it to be reliable, with units sold to customers over the years performing well under real-life conditions.” • Explanation – Because of plasticity effects, Be foil withstands 1 Atm (according to BW tests) even if Roark’s calculation says that it doesn’t withstand Michael MONTEIL - 12 April 2010 Data: Brush Wellman 18 To know • Be have ultra high resistance to fatigue cracking • High endurance strength level Michael MONTEIL - 12 April 2010 Data: Brush Wellman 19 Solutions #5 stresses and deflection - C-C+Be under DP = 1 atm • Linear circular fixed support • 2 planes of symmetry • Geometry – Diameter f 80 mm – Thickness: 0.254 mm – Aperture: f 60 mm • Pressure 1 atm Michael MONTEIL - 12 April 2010 20 ANSYS Study - Solutions #5 stresses and deflection - C-C+Be under DP = 1 atm • Beryllium foil study – Smooth and continuous temperature distribution – Through-thickness energy deposition – Coefficient of Thermal Expansion varying with temperature – Be (pure elasticity): • Poisson’s ratio = 0.08 • High Re = 303 Mpa Michael MONTEIL - 12 April 2010 21 Michael MONTEIL - 12 April 2010 22 Michael MONTEIL - 12 April 2010 23 Michael MONTEIL - 12 April 2010 24 Michael MONTEIL - 12 April 2010 25 Michael MONTEIL - 12 April 2010 26 Michael MONTEIL - 12 April 2010 27 Michael MONTEIL - 12 April 2010 28 Michael MONTEIL - 12 April 2010 29 Michael MONTEIL - 12 April 2010 30 Michael MONTEIL - 12 April 2010 31 Michael MONTEIL - 12 April 2010 32 Conclusion: influence of gap reducing • So if we flatter the foil on the C-C, we reduce the Max stress (as shows ANSYS calculation with non plasticity model), maybe also stay in elastic domain (Bellow 275Mpa at room Temp). We will manage to reduce this gap (flattering the Be foil as much as possible on C-C plate) Michael MONTEIL - 12 April 2010 33 Easiness to reduce Gap C-C / Be Option 1 Option 2 Michael MONTEIL - 12 April 2010 34 To do : • Order Beryllium – Delivery: 4 Weeks ARO for flanges (Option 1) – Delivery: 6 Weeks ARO fro foil (Option 2) • Assembly • Test Michael MONTEIL - 12 April 2010 35 Michael MONTEIL - 12 April 2010 36 V2.0 slides Michael MONTEIL - 12 April 2010 37 Window geometry – C-C option • Carbon/Carbon composite: 1501 G from SGL • Cylindrical window • Diameter f 80 mm – Aperture f 60 mm • Thickness: 0.5 cm • Aperture (flange internal diameter): f 60 mm Michael MONTEIL - 12 April 2010 38 Solutions #1 for C-C tightness problem: Differential vacuum (V2.0) • 1 Window C-C – Pumping speed needed: 2.3x108 l/s … • 2 Windows C-C with differential pumping – Pumping speed needed: 8.94x102 l/s OK ! • 3 Windows C-C with differential pumping – Pumping speed needed: 13 l/s Too low ?! Michael MONTEIL - 12 April 2010 39 Solutions #1 • What about radiations in this area ? – Possible maintenance needed on the roots pump… • Protective atmosphere • Decreasing pressure in Vacuum side with serial pumps Michael MONTEIL - 12 April 2010 40 P1 (ATM) Window1 1.00E+03 P D cm C-C 6 6 K cm2/s 5.00E-02 5.00E-02 A cm2 L cm 2.83E+01 0.5 2.83E+01 0.5 Q mbar*cm3/s 2.83E+00 8.94E-06 1.00E+03 3.16E-03 DP mbar 3 Q mbar*cm /s S m3/h P1 (ATM) Window1 1.00E+03 D cm A cm2 L cm 2.83E+01 0.5 2.83E+01 0.5 Q mbar*cm3/s 2.83E+00 2.83E-05 1.00E+03 1.00E-02 2.83E+00 2.83E-05 S l/s m3/h P1 (ATM) Window1 1.00E+03 P D cm 2.83E+01 0.5 2.83E+01 0.5 Q mbar*cm3/s 2.83E+00 8.94E-05 1.00E+03 3.16E-02 2.83E+00 8.94E-05 S l/s m3/h 2.83E+00 1.41E-05 1.00E+03 5.00E-03 2.83E+00 1.41E-05 l/s m3/h P1 (ATM) Window1 1.00E+03 P 5.65E+02 1413.714 2035.7 5089.4 P2 Window2 P3 3.16E-03 1.00E-08 6 6 K cm2/s 5.00E-02 5.00E-02 A cm2 L cm 2.83E+01 1 2.83E+01 1 Q mbar*cm3/s 1.41E+00 4.47E-06 1.00E+03 3.16E-03 1.41E+00 4.47E-06 Q mbar*cm /s S l/s m3/h 4.47E+02 447.0551 1609.4 1609.4 P2 Window2 P3 3.16E-02 1.00E-06 A cm L cm Q mbar*cm /s Q mbar*cm3/s 3 1017.9 6 3 2.83E+01 0.5 DP mbar 1017.9 5.00E-02 DP mbar 2.83E+01 0.5 S C-C 282.7405 6 2 A cm2 L cm D cm 2.83E+02 5.00E-02 K cm2/s 6 5.00E-02 Q mbar*cm /s P2 Window2 P3 1.00E-02 1.00E-07 5.00E-02 6 5.00E-02 3 3218.8 P2 Window2 P3 5.00E-03 1.00E-08 K cm2/s DP mbar 894.1101 5.00E-02 Q mbar*cm3/s C-C 3218.8 K cm /s DP mbar D cm 8.94E+02 6 P1 (ATM) Window1 1.00E+03 P 8.94E-06 6 2 C-C 2.83E+00 l/s P C-C P2 Window2 P3 3.16E-03 1.00E-08 Reference 8.94E+01 89.40847 321.87 321.87 • P2 : Roots pump • 100 –> 1500 m3/h • 10-3 -> 10 Bar • P3 : Ion pump • 400 l/s Michael MONTEIL - 12 April 2010 41 Solutions #2 for C-C tightness problem: Add a Graphite foil (v1.0) Solution #3 : Tight steel“ring” with a C-C plate (v1.0) Solution #4 : Beryllium Michael MONTEIL - 12 April 2010 42 Michael MONTEIL - 12 April 2010 43 ANSYS Study - Solutions #1 stresses and deflection - C-C under DP = 1.4atm • Linear circular fixed support • 2 planes of symmetry • Geometry – Diameter f 80 mm – Thickness: 5 mm – Aperture: f 60 mm • Pressure 1.4 bar Michael MONTEIL - 12 April 2010 44 ANSYS Study - Solutions #1 stresses and deflection - C-C under DP = 1.4atm • Orthotropic properties : 18 plies [0°/90°…] • Smooth and continuous temperature distribution • Through-thickness energy deposition • Coefficient of Thermal Expansion varying with temperature and directions Michael MONTEIL - 12 April 2010 45 C-C - Pressure load - Deflection 7.4 μm Michael MONTEIL - 12 April 2010 46 C-C - Pressure load – Von-Mises 5.9 Mpa Michael MONTEIL - 12 April 2010 47 C-C - Pressure load – Tsaï-Wu Michael MONTEIL - 12 April 2010 48 C-C - Thermal load ANSYS input = FLUKA output C-C | 1s = 0.5 mm | 1.7e11 p+ | 288 bunches • Axisymmetrical radial temperature field T (°C) T (°C) R (cm) Radial Z (cm) Depth Michael MONTEIL - 12 April 2010 49 C-C - Pressure + Thermal load – Deflection 10.6 μm Michael MONTEIL - 12 April 2010 50 C-C - Pressure + Thermal load – Von-Mises 31 Mpa Michael MONTEIL - 12 April 2010 51 C-C - Pressure + Thermal load – TsaïWu Michael MONTEIL - 12 April 2010 52 Michael MONTEIL - 12 April 2010 53 ANSYS Study - Solutions #4 stresses and deflection - Be under DP = 1.4atm • Linear circular fixed support • 2 planes of symmetry • Geometry – Diameter f 80 mm – Thickness: 0.254 mm – Aperture: f 60 mm • Pressure 1.4 bar Michael MONTEIL - 12 April 2010 54 ANSYS Study - Solutions #4 stresses and deflection - Be under DP = 1.4atm • Smooth and continuous temperature distribution • Through-thickness energy deposition • Coefficient of Thermal Expansion varying with temperature • Be: – Poisson’s ratio = 0.1 – High Re = 275 Mpa – High Rm = 551 MPa Michael MONTEIL - 12 April 2010 55 Be - Pressure load - Deflection 0.81 mm Michael MONTEIL - 12 April 2010 56 Be - Pressure load – Von-Mises 319 Mpa Michael MONTEIL - 12 April 2010 57 Be - Pressure load – Safety factor Ult. Strength 1.7 Michael MONTEIL - 12 April 2010 58 Be - Thermal load ANSYS input = FLUKA output Be | 1s = 0. 5 mm | 1.7e11 p+ | 288 bunches • Axisymmetrical radial temperature field T (°C) T (°C) Z (cm) Radial Be Z (cm) Michael MONTEIL - 12 April 2010 59 Be - Pressure + Thermal load – Deflection 0.8 mm Michael MONTEIL - 12 April 2010 60 Be - Pressure + Thermal load – Von-Mises 315 Mpa Michael MONTEIL - 12 April 2010 61 Be - Pressure + Thermal load – Safety factor Ult. Strength 1.7 Michael MONTEIL - 12 April 2010 62 ANSYS Study - Solutions #5 • stresses and deflection - C-C+Be under DP = 1.4atm 2 Studies – C-C (See Solution #4) • • Pressure load Pressure + Temperature loads – Be (Following slides) • • • • Flattered on a C-C plate (Fixed support) and apply pressure load on the other side Flattered on a C-C plate (Fixed support) and apply pressure load on the other side + Temperature load 2 planes of symmetry Geometry – Diameter f 80 mm – Thickness • • C-C: 5 mm Be: 0.254 mm – Aperture: f 60 mm • Pressure 1.4 bar Michael MONTEIL - 12 April 2010 63 ANSYS Study - Solutions #5 stresses and deflection - C-C+Be under DP = 1.4atm • Smooth and continuous temperature distribution • Through-thickness energy deposition • Coefficient of Thermal Expansion varying with temperature Michael MONTEIL - 12 April 2010 64 Be (flatter on C-C) - Pressure load – Deformation Michael MONTEIL - 12 April 2010 65 Be (flatter on C-C) - Pressure load – Von-Mises Michael MONTEIL - 12 April 2010 66 Thermal load ANSYS input = FLUKA output C-C + Be | 1s = 0.5 mm | 1.7e11 p+ | 288 bunches • Axisymmetrical radial temperature field T (°C) T (°C) Depth C-C Z (cm) Z (cm) Radial C-C Z (cm) Radial Be Michael MONTEIL - 12 April 2010 67 Be (flatter on C-C) - Pressure + Thermal load – Deflection 5.4 um x 2.6e+002 Michael MONTEIL - 12 April 2010 68 Be (flatter on C-C) - Pressure + Thermal load – Von-Mises Michael MONTEIL - 12 April 2010 69 Be (flatter on C-C) - Pressure + Thermal load – Safety factor Ult. Strength x 2.6e+002 Michael MONTEIL - 12 April 2010 70 To do : • Rough mechanical design – Solution #1 C-C with differential pumping • Maybe coating • 15 cm length between upstream and downstream sides – Solution #5 C-C + Be • Order quotes of Be • Same design that window in TI8, TI2, TT41 (Design by Kurt Weiss, Luca Bruno and Jose Miguel Jimenez) but replacing the Ti foil by a Be foil • Nickel-coating to prevent oxidation on Be ? • 15 cm length between upstream and downstream sides Michael MONTEIL - 12 April 2010 71