The fabrication fidelity and vacuum properties are tested for currently
available 3D-printed materials including polyamide, glass, acrylic, and
sterling silver. The silver was the only material found to be suitable to
ultrahigh vacuum environments due to outgassing and sublimation observed in
other materials.Comment: 3 pages, 2 figures, preprin

Alexander P. Povilus

Caroline J. Wurden

Govett T.

Joel Fajans

Marcelo Baquero-Ruiz

Zak Vendeiro

English

arXiv

The fabrication fidelity and vacuum properties are tested for currently available 3D-printed materials including polyamide, glass, acrylic, and sterling silver. The silver was the only material found to be suitable to ultrahigh vacuum environments due to outgassing and sublimation observed in other materials. © 2014 American Vacuum Society

Povilus, Alexander P

Wurden, Caroline J

Vendeiro, Zak

Baquero-Ruiz, Marcelo

Fajans, Joel

eScholarship - University of California

UC BerkeleyUC Berkeley Previously Published WorksTitleVacuum compatibility of 3D-printed materialsPermalinkhttps://escholarship.org/uc/item/6s17p4jnJournalJournal of Vacuum Science & Technology A Vacuum Surfaces and Films, 32(3)ISSN0734-2101AuthorsPovilus, Alexander PWurden, Caroline JVendeiro, Zaket al.Publication Date2014-05-01DOI10.1116/1.4873556 Peer reviewedeScholarship.org Powered by the California Digital LibraryUniversity of CaliforniaVacuum Compatibility of 3D-Printed MaterialsA. P. Povilus,1 C. J. Wurden,1 Z. Vendeiro,1 M. Baquero-Ruiz,1 and J. Fajans11Department of Physics, University of California at Berkeley, Berkeley, CA 94720-7300, USA∗(Dated: September 16, 2013)The fabrication fidelity and vacuum properties are tested for currently available 3D-printed mate-rials including polyamide, glass, acrylic, and sterling silver. The silver was the only material foundto be suitable to ultrahigh vacuum environments due to outgassing and sublimation observed inother materials.I. INTRODUCTIONAdditive manufacturing, or 3D printing, of parts hasmany potential advantages over traditional machining forconstruction of experimental apparati.1 Material and ma-chining costs of parts fabricated using 3D-printing meth-ods are generally lower since there is little waste in theprocess and complicated shapes become much easier toproduce. Printing also gives the ability to generate ge-ometries that would have only been previously possi-ble with either welding or an expensive casting process.Since printing is additive, it is possible that there aresmall voids in the material that would trap gases thatwould later vent slowly into the vacuum, making the partunsuitable for ultrahigh vacuum environments.2 It is ofparticular interest how well these materials perform ina vacuum environment since they can drastically reducethe time and cost to build complicated, specialized ge-ometries, such as resonant electrode strucutres, for usein cold atom traps and plasma devices.II. PRINTED PART DESCRIPTIONIn order to test the dimensional tolerances and out-gassing properties of printed materials, a CAD designfor a modified waveguide was printed by Shapeways ina variety of different materials using printers developedby EOS GmbH.3 These printers use a technique calledselective laser sintering (SLS) to fuse powdered materi-als into parts.4 While the waveguides were ordered froma specific printing service, they are thought to be rep-resentative of 3D printed materials by examination ofmaterial datasheets from similar sintering printer ser-vices that use the same methods. The waveguide wasmodified to include extra exterior tabs to measure di-mensional tolerances of the printing process. Printedmaterials included glass, acrylic, PA12 polyamide, alu-mide (polyamide/aluminum powder), and sterling silver(92.5% Ag). Although stainless steel was also available,we did not use it in our system since it was found to be ahighly-magnetic alloy incompatable with magnetic con-finement experiments of interest to us. It is important tonote that sterling silver printing is a cast part where themold has been 3D printed, so it is not expected to havetrapped gases that the other materials may have.Anomalies in the printed parts were noted for these3,541,2,5FIG. 1. (Color online) CAD renditions ( top left) of a modi-fied waveguide used as an sample 3D printed part compareda photograph (bottom left) of the actual waveguide printedin sterling silver. The lengths of particular features of thiswaveguide, highlighted in the CAD renders, are comparedto printed versions of waveguide in different materials. Thedifference of the measured length of each waveguide to thenominal length in the CAD submission is shown for thesefeatures in the graph. (right) The waveguide has dimensions48mm×20mm×19mm. Measurements were made to 0.01mmaccuracy and precision..waveguides. Glass was found to be unsuitable for finedetail, as it warped significantly such that surfaces de-signed to be flat became noticeably concave (> 0.5mmdeflection), even with sufficient support during printing.Common failure modes in others materials included mi-nor distortions in thickness or breaks, especially in a thintab (0.65mm) designed to test fabrication of small fea-tures. At the present, fractures and poor resolution inthin features is a known issue with printing fine-detailedobjects fabricated by a laser sintering process.5 The thinacrylic tab broke off at the base during shipping and thesilver tab, while solidly attached, had a small fracturerunning through the material. The adjacent, thicker tab(1.29mm) did not have these defects in either the silveror acrylic. The printed silver and acrylic were found tohave excellent machinability, so some small features mayarXiv:1308.4962v2  [physics.ins-det]  12 Sep 20132FIG. 2. Residual gas analysis of materials in a vacuum system24 hours after cleaning and bakeout processes. The top curveis the residual gas of an empty chamber.still be possible by traditional machining methods afterprinting an oversized piece.The accuracy and precision of printed part dimensionswas measured by comparing the lengths of features onthe waveguide to the nominal specifications in the CADmodel. The difference between the nominal and mea-sured lengths are compared in Fig. 1. Note that the silverpart was found to be scaled down by ∼ 1.6% relative tothe CAD model; this was confirmed by the printing ser-vice to be a miscalibration of the scaling in the printer.In order to compensate for this, we measured accuracy asthe variance from the residual sum of squares assuminga linear offset. The accuracy was found to be ±0.072mmand ±0.138mm for silver and polyamide respectively.III. VACUUM PROPERTIESBefore measuring the outgassing behavior of the mate-rials, the waveguides were chemically cleaned and bakedin vacuum to remove any oils or dust. Using CERN clean-ing guidelines,6 adapted as needed to suit the variety ofmaterials, the following general procedure was used toclean parts:1. Ultrasonically clean part in deionized water withmild detergent2. Rinse with deionized water3. Degrease using acetone if material is acetone resis-tant4. Ultrasonically clean with ethanol heated at 40C todissolve excess organics5. Evaporate excess ethanol by spraying with dry ni-trogen6. Insert into vacuum chamber and pump down to10−6 mbar or better pressure7. Bake chamber at 24 hours at minimum of either120◦C or maximum recommended temperature ofthe material. Ramp temperatures up and down ata maximum of 5C/hr.The baking and residual gas analysis was performed inthe same vacuum chamber. The 25L, room-temperaturevacuum chamber was brought to ultrahigh vacuum by aturbopump backed by a dry rotary roughing pump andmaintained using an 150L/s ion pump. The empty cham-ber was able to be pumped to an ultimate pressure of2.0 · 10−9 mbar. With the gas analyzer filament on, theempty chamber pressure rose to 1.2 · 10−8 mbar, wherenearly 90% of the total pressure is due to molecular hy-drogen. This is a typical behavior found in hot-filamentvacuum gauges such as the gas analyzer due to adsorp-tion processes.7The residual gas analysis was performed using a SRSRGA100 mass spectrometer 24 hours after the bakeoutwas completed. The spectrometer filament was placedout of line of sight of the test piece to avoid excess heat-ing; results are shown in Fig. 2. The silver piece had out-gassing rates below 1×10−10mbar L/cm2s, the detectionlimit of our analyzer. The polyamide and alumide hadoutgassing rates of ∼ 3×10−8−4×10−7mbar L/cm2s fol-lowing baking, comparable to teflon and viton materials.8The residual gases present were atmospheric, suggest-ing that air was trapped in the material. Alumide, al-though part polyamide, appears to have adsorpted lesswater from the cleaning process. To avoid sublimationof polyamide material itself, the polyamide based mate-rials must be baked at a low temperature (65◦C). Whenattempts were made to bake at 100◦C, the vacuum be-came very poor (∼ 10−6mbar) and a residue was foundon the vacuum chamber walls near the piece. Glass hadoutgassing performance comparable with the polyamidematerials, but could be baked at higher temperatures.Acrylic was not able to be pumped to ultrahigh vac-uum pressure levels. The mass spectrum for acrylic ap-pears to have a hydrocarbon chain contamination, shownas the 13amu repeating feature in the mass spectrum,leading to the conclusion the acrylic material was subli-mating into vacuum, even at low (55◦C) baking temper-atures.3IV. CONCLUSIONOf the tested materials, only sterling silver wasfound to be accurately printed and UHV-compatible;polyamide-based materials could be used sparingly invacuum similar to teflon and viton. Glass and acrylicare not recommended since glass tended to deform dur-ing fabrication, and acrylic had very poor bakeout per-formance.∗ povilus@berkeley.edu1 Journal of Microscopy, 169, 383389 (1993)2 JOM,50 12, 17-20(1998)3 MSDS and Property Datasheets for materials avail-able at http://www.shapeways.com/ and http://eos.materialdatacenter.com/.4 C. Deckard, ”Method and apparatus for producing parts byselective sintering”, US Patent 4863538A5 T. Govett, K. Kim, M. Lundin and D. Pinero, in ”De-sign Rules For Selective Laser Sintering” at MechanicalEngineering Design Projects Program, The University ofTexas at Austin (2012) Available at www.me.utexas.edu/~ppmdlab.6 Taborelli, M, in CAS - CERN Accelerator School and ALBASynchrotron Light Facility : Course on Vacuum in Acceler-ators, Platja d’Aro, Spain (2006), p.321.7 P. A. Redhead, J. Vac. Sci. Technol. A 5, 3215 (1987).8 R. N. Peacock, J. Vac. Sci. Technol., 17, 330 (1980).

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