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1

Littaye, Alexandra Zelda. "The multifunctionality of heritage food: The example of pinole, a Mexican sweet." Geoforum 76 (November 2016): 11–19. http://dx.doi.org/10.1016/j.geoforum.2016.08.008.

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2

Littaye, Alexandra. "The role of the Ark of Taste in promoting pinole, a Mexican heritage food." Journal of Rural Studies 42 (December 2015): 144–53. http://dx.doi.org/10.1016/j.jrurstud.2015.10.002.

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3

Méndez-Albores, A., F. De Jesús-Flores, E. Castañeda-Roldan, G. Arámbula-Villa, and E. Moreno-Martı́nez. "The effect of toasting and boiling on the fate of B-aflatoxins during pinole preparation." Journal of Food Engineering 65, no. 4 (December 2004): 585–89. http://dx.doi.org/10.1016/j.jfoodeng.2004.02.024.

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4

Gallegos-Infante, José A., Nuria E. Rocha-Guzman, Ruben F. Gonzalez-Laredo, and Mayra A. Garcia-Casas. "Efecto del procesamiento térmico sobre la capacidad antioxidante de pinole a base de vainas de mezquite (Prosopis laevigata)." CyTA - Journal of Food 11, no. 2 (May 2013): 162–70. http://dx.doi.org/10.1080/19476337.2012.712057.

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5

Golesorkhie, Farya, and Mani Navi. "Effects of geometric variations on buckling properties of carbon nanostructures: A finite element analysis." Journal of Mechanical Engineering and Sciences 14, no. 1 (March 23, 2020): 6473–87. http://dx.doi.org/10.15282/jmes.14.1.2020.22.0507.

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Critical Bucking Load (CBL) is one of the essential parameters to describe the mechanic stabilities of materials, e.g. the low-dimensional carbon nanostructures. While the CBL of pristine carbon nanotubes have been previously investigated using the quantum mechanics-based calculations, the effect of geometrical variation on the CBL of carbon nanomaterials is rarely reported since it need considerably large atomic models, which needs high computational cost. In this study, both the analytical and Finite Element (FE) methods were employed to systematically explore the impact of atomic vacancies, shapes and heterostructures on the CBLs of carbon nanomaterials with the acceptable computational cost. Our studies on the pristine CNTs first demonstrate the validity of the method we used. After that, the systems with mono-/bi-/tri-/pinole-vacancies either on nanocones, nanotube, linearly-joined nanotubes or angle-adjoined were simulated and analyzed. Our results reveal that the CBL values decrease with the increase of the aspect ratio of all considered nanomaterials. Based on the obtained results, the CBL of nanocone with the aspect ratio of 1, reduces significantly, from 50 nN to 10 nN when the aspect ratio is 3. The CBL of homogeneous, capped, and joint CNTs reduces to below 2 nN when the aspect ratio is above 14. The introduction of geometric variations can greatly affect the CBL values. The larger atomic vacancy has more serious impact on the CBLs. The most highlighted impact is for the pinhole vacancy where the CBL reduces to up to 70% of the original value. Our studies on linearly-joint and angle-joint carbon hybrids further demonstrate that the CBL can also be affected by the boundary conditions and joint structures of the hybrids.
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6

Carrera, Y., R. Utrilla-Coello, A. Bello-Pérez, J. Alvarez-Ramirez, and E. J. Vernon-Carter. "In vitro digestibility, crystallinity, rheological, thermal, particle size and morphological characteristics of pinole, a traditional energy food obtained from toasted ground maize." Carbohydrate Polymers 123 (June 2015): 246–55. http://dx.doi.org/10.1016/j.carbpol.2015.01.044.

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7

Hu, Shunyou, Linlin Wang, Xiaopeng Chen, Xiaojie Wei, Zhangfa Tong, and Lijiang Yin. "The conversion of α-pinene to cis-pinane using a nickel catalyst supported on a discarded fluid catalytic cracking catalyst with an ionic liquid layer." RSC Advances 9, no. 11 (2019): 5978–86. http://dx.doi.org/10.1039/c9ra00675c.

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8

Wiberg, Kenneth B., Yi-gui Wang, Michael J. Murphy, and Patrick H. Vaccaro. "Temperature Dependence of Optical Rotation: α-Pinene, β-Pinene Pinane, Camphene, Camphor and Fenchone." Journal of Physical Chemistry A 108, no. 26 (July 2004): 5559–63. http://dx.doi.org/10.1021/jp040085g.

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9

Sol Sánchez, Ángel, José Alberto Naranjo González, Víctor Córdova Avalos, Dora Angélica Ávalos de la Cruz, and Juan Manuel Zaldívar Cruz. "Caracterización bromatológica de los productos derivados de cacao (Theobroma cacao L.) en la Chontalpa, Tabasco, México." Revista Mexicana de Ciencias Agrícolas, no. 14 (November 3, 2017): 2817. http://dx.doi.org/10.29312/remexca.v0i14.453.

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La Norma Mexicana NMX-F-061-1964, especifica las características fisicoquímicas de los chocolates de mesa y los clasifica en tres tipos: chocolate amargo, chocolate semi-amargo y chocolate dulce. Conocer y especificar la composición de un producto alimenticio es importante ya que nos permite tener un control de la calidad, valorar su contenido nutricional, dar confianza al consumidor, además de ser un requisito de etiquetado en los productos derivados de cacao. El objetivo de este estudio fue caracterizar la calidad fisicoquímica de los productos tradicionales y no tradicionales derivados del cacao de la región de la Chontalpa, Tabasco. Se consideraron cuatro parámetros: materia grasa (G) por el método Soxhlet, proteína (P) usando el método Kjeldahl, cenizas (C) por incineración en la muf la y humedad (H) por pérdida de peso en estufa. Se evaluaron 32 muestras de productos elaborados a base de cacao en la región, de los cuales 13 tipos de chocolate y 19 de polvillo. Los resultados nos permitieron clasificar los productos con la siguiente composición: los chocolates amargos, G de 40.87 a 48.18%, P de 8.75%, C de 2.60 a 4.42% y H de 1.63 a 1.97%; los chocolates semi-amargos, G de 30.33 a 44.68%, P de 8.75%, C de 1.59 a 4.08% y H de 2.37 a 8.01%; los chocolates dulces, G de 9.66 a 30.35%, P de 8.75%, C de 1.31 a 3.56% y H de 1.18 a 6.88%; los polvillos de cacao y pinole, G de 3.07 a 5.06%, P de 8.75%, C de 1.67 a 4.89% y H de 5.70 a 7.28%; los polvillos de dos ingredientes, G de 10.20 a 34.57%, P de 8.75%, C de 1.89 a 7.69% y H de 5.78 a 7.45%; y finalmente, lo chocolates con alto contenido de azúcar (muy dulces), G de 5.68 a 11.7%, P de 8.75%, C de 2.13 a 7.69% y H de 3.88 a 7.02%. Los resultados obtenidos fueron comparados con los estándares especificados en la Normas Mexicanas y el Codex Alimentarius.
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10

Wang, Congmin, Haoran Li, Lu Ma, and Shijun Han. "(Vapour+liquid) equilibria for the binary mixtures (cis-pinane+α-pinene) and (cis-pinane+1-butanol)." Journal of Chemical Thermodynamics 35, no. 1 (January 2003): 131–36. http://dx.doi.org/10.1016/s0021-9614(02)00309-9.

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11

Green, F. B., T. J. Lundquist, and W. J. Oswald. "Energetics of advanced integrated wastewater pond systems." Water Science and Technology 31, no. 12 (June 1, 1995): 9–20. http://dx.doi.org/10.2166/wst.1995.0448.

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An energy balance is presented for a second generation Advanced Integrated Wastewater Pond System (AIWPS) prototype at the University of California, Berkeley, Environmental Engineering and Health Sciences Laboratory in Richmond, California. Modifications were made to the existing 1.8 ML facultative pond in order to further optimize methane fermentation and to demonstrate the recovery of methane using a submerged gas collector. Methane production rates were determined over a range of in-pond digester loadings and temperatures. The feasibility of submerged gas collection was proven, and the advantages of in-pond digestion in terms of BOD5 and VSS removal as well as biogas scrubbing were quantified. Biogas methane concentrations increased by more than 50% as the biogas emerged through the overlying water column and most of the carbon dioxide fraction was utilized by microalgae. Electrical power requirements for mixing two 0.1 hectare algal High Rate Ponds (HRPs) were measured over a range of channel depths and velocities, and electrical power requirements for daily recirculation pumping were also measured. Oxygenation and total treatment energy requirements for the second generation AIWPS prototype at Richmond were compared with oxygenation and total treatment energy requirements for the first generation AIWPS at St. Helena, California and for two mechanical wastewater treatment plants of comparable capacity and effluent quality at Pinole and Brentwood, California. Using preliminary methane production and recovery rates achieved at Richmond, the cogeneration potential was estimated and projected for larger second generation AIWPSs of 2 MLD and 200 MLD capacities. By incorporating methane recovery and electrical power generation together with efficient HRP mixing using paddle wheels, full-scale second generation AIWPSs will be able to produce as much energy as they require for primary and secondary treatment. Additional energy would be required to produce a tertiary disinfected effluent suitable for unrestricted reuse in California, including recreational and indirect potable reuse. The additional power requirements for complete algal harvest using dissolved air flotation (DAF) and filtration were estimated for second generation AIWPSs based on data collected at Richmond and Stockton, California, and the additional power requirements for final UV disinfection were estimated.
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12

Qu, Xinhua, Eunah Lee, Gu-Sheng Yu, Teresa B. Freedman, and Laurence A. Nafie. "Quantitative Comparison of Experimental Infrared and Raman Optical Activity Spectra." Applied Spectroscopy 50, no. 5 (May 1996): 649–57. http://dx.doi.org/10.1366/0003702963905970.

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Infrared vibrational circular dichroism (VCD) and vibrational Raman optical activity (ROA) have been measured and compared quantitatively over the frequency range from 835 to 1345 cm−1 for trans-pinane, cis-pinane, α-pinene, and β-pinene. For these molecules in this region of spectral overlap between VCD and ROA, the average ratio of VCD or ROA to its parent vibrational intensity favors ROA by a factor of two to three. Several vibrational modes in each molecule yield both large VCD and large ROA, while several other modes show little propensity toward significant VCD or ROA intensity. Beyond this general property of a few strongly chiral and strongly achiral vibrational modes, little additional correlation between VCD and ROA intensity is found. This quantitative compilation of VCD, infrared, ROA, and Raman intensities provides an experimental basis for computational intensity studies of VCD, ROA, and their theoretical comparison.
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13

Bader, Ammar, Pier Luigi Cioni, and Guido Flamini. "GC-MS Analysis of the Essential Oils of Ripe Fruits, Roots and Flowering Aerial Parts of Elaeoselinum asclepium subsp. meoides growing in Sicily." Natural Product Communications 5, no. 7 (July 2010): 1934578X1000500. http://dx.doi.org/10.1177/1934578x1000500727.

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The compositions of the essential oils obtained by hydrodistillation of the ripe fruits, flowering aerial parts and roots of Elaeoselinum asclepium (L.) Bertol subsp. meoides (Desf.) Fiori (Apiaceae) were determined by GC-MS analysis. All the analyzed parts were very rich in α-pinene (77.1%, 92.2% and 60.8%, respectively). Other compounds detected in appreciable amounts were β-pinene (4.3%, 4.0% and 8.2%), and sabinene (11.9% in ripe fruits; 12.8% in aerial parts). The plant synthesizes different classes of monoterpenes, including pinane, camphane, thujane, menthane, and fenchane derivatives, besides some acyclic monoterpenes. Trace amounts of sesquiterpenes and diterpenes were also detected.
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14

Bajtel, Ákos, Mounir Raji, Matti Haukka, Ferenc Fülöp, and Zsolt Szakonyi. "Stereoselective synthesis and transformation of pinane-based 2-amino-1,3-diols." Beilstein Journal of Organic Chemistry 17 (May 3, 2021): 983–90. http://dx.doi.org/10.3762/bjoc.17.80.

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A library of pinane-based 2-amino-1,3-diols was synthesised in a stereoselective manner. Isopinocarveol prepared from (−)-α-pinene was converted into condensed oxazolidin-2-one in two steps by carbamate formation followed by a stereoselective aminohydroxylation process. The relative stereochemistry of the pinane-fused oxazolidin-2-one was determined by 2D NMR and X-ray spectroscopic techniques. The regioisomeric spiro-oxazolidin-2-one was prepared in a similar way starting from the commercially available (1R)-(−)-myrtenol (10). The reduction or alkaline hydrolysis of the oxazolidines, followed by reductive alkylation resulted in primary and secondary 2-amino-1,3-diols, which underwent a regioselective ring closure with formaldehyde or benzaldehyde delivering pinane-condensed oxazolidines. During the preparation of 2-phenyliminooxazolidine, an interesting ring–ring tautomerism was observed in CDCl3.
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15

Erman, Mark B, and Bernard J Kane. "Chemistry Around Pinene and Pinane: A Facile Synthesis of Cyclobutanes and Oxatricyclo‐Derivative of Pinane fromcis‐ andtrans‐Pinanols." Chemistry & Biodiversity 5, no. 6 (June 2008): 910–19. http://dx.doi.org/10.1002/cbdv.200890104.

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16

Barron, L. D., L. Hecht, A. R. Gargaro, and W. Hug. "Vibrational Raman optical activity in forward scattering: Trans-pinane and β-pinene." Journal of Raman Spectroscopy 21, no. 6 (June 1990): 375–79. http://dx.doi.org/10.1002/jrs.1250210609.

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17

lin, Yingrui, Dawei Ma, and Xiyan Lu. "Selective cconversion of pinane into β-pinene catalyzed by an iridium pentahydride complex." Journal of Organometallic Chemistry 323, no. 3 (April 1987): 407–9. http://dx.doi.org/10.1016/0022-328x(87)80434-5.

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18

Bartlett, Albert A. "Pinhole mirror." Physics Teacher 34, no. 8 (November 1996): 479. http://dx.doi.org/10.1119/1.2344536.

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19

Renner, Eric. "Pinhole Photography." History of Photography 9, no. 4 (October 1985): 330. http://dx.doi.org/10.1080/03087298.1985.10443038.

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20

Colicchia, Giuseppe, Martin Hopf, Hartmut Wiesner, and Dean Zollman. "Pinhole Glasses." Physics Teacher 46, no. 1 (January 2008): 26–28. http://dx.doi.org/10.1119/1.2823996.

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21

Patera, Russell. "Pinhole glasses?" Physics Teacher 44, no. 2 (February 2006): 122. http://dx.doi.org/10.1119/1.2165448.

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22

Bouř, Petr, Vladimír Baumruk, and Jana Hanzlíková. "Measurement and Calculation of the Raman Optical Activity of α-Pinene and trans-Pinane." Collection of Czechoslovak Chemical Communications 62, no. 9 (1997): 1384–95. http://dx.doi.org/10.1135/cccc19971384.

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Raman scattering and Raman optical activity (ROA) spectra of α-pinene and trans-pinane were measured for both enantiomers. The experiment was performed on a newly built, fully computer-controlled backscattering incident circular polarization ROA instrument. High-quality spectra were obtained and interpreted on the basis of ab initio quantum chemical calculations. Excellent agreement between the calculated and observed spectra was observed in the mid IR region. An approximate distributed origin gauge model for calculation of the polarization tensors was proposed. The shapes of ROA spectra calculated with this model are similar to those obtained with conventional, computationally more demanding ROA computations.
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23

Tai, Y. C., H. Wu, D. Pal, and J. A. O'Sullivan. "Virtual-Pinhole PET." Journal of Nuclear Medicine 49, no. 3 (February 20, 2008): 471–79. http://dx.doi.org/10.2967/jnumed.107.043034.

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24

Young, Jay A. "A pinhole leak." Chemical Health and Safety 9, no. 2 (March 2002): 5. http://dx.doi.org/10.1016/s1074-9098(02)00285-x.

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25

Ambrosini, D., and G. Schirripa Spagnolo. "Successful pinhole photography." American Journal of Physics 65, no. 3 (March 1997): 256–57. http://dx.doi.org/10.1119/1.18538.

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26

Hofeldt, Albert J., and Michael J. Weiss. "Potential acuity pinhole." Ophthalmology 107, no. 4 (April 2000): 623–24. http://dx.doi.org/10.1016/s0161-6420(99)00159-1.

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27

Melki, Samir A., Ammar Safar, John Martin, Anastasia Ivanova, and Marwa Adi. "Potential acuity pinhole." Ophthalmology 106, no. 7 (July 1999): 1262–67. http://dx.doi.org/10.1016/s0161-6420(99)00706-x.

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28

Pasachoff, Jay M. "ECLIPSE PINHOLE IMAGES." American Journal of Physics 82, no. 4 (April 2014): 269. http://dx.doi.org/10.1119/1.4864639.

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29

Lancor, Rachael, and Brian Lancor. "Digital Pinhole Camera." Physics Teacher 52, no. 9 (December 2014): 546–47. http://dx.doi.org/10.1119/1.4902199.

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30

Gardner, Martin. "A pinhole paradox." Physics Teacher 38, no. 6 (September 2000): 372. http://dx.doi.org/10.1119/1.1531560.

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31

Gude, Tore. "Err’u pingle, eller?" Tidsskrift for Den norske legeforening 133, no. 19 (2013): 2068. http://dx.doi.org/10.4045/tidsskr.13.0939.

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32

Wang, Guiying, Yanling Zheng, Aimin Sun, Shudong Wu, and Zhijiang Wang. "Polarization pinhole interferometer." Optics Letters 16, no. 17 (September 1, 1991): 1352. http://dx.doi.org/10.1364/ol.16.001352.

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33

Boland, Eavan. "The Pinhole Camera." Yale Review 90, no. 1 (January 2002): 20–21. http://dx.doi.org/10.1111/0044-0124.00570.

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34

Hou, Shengli, Congxia Xie, Fengli Yu, Bing Yuan, and Shitao Yu. "Selective hydrogenation of α-pinene to cis-pinane over Ru nanocatalysts in aqueous micellar nanoreactors." RSC Advances 6, no. 60 (2016): 54806–11. http://dx.doi.org/10.1039/c6ra13099b.

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35

Cantiani, P., U. Di Salvatore, and R. Romano. "Silvicultural aspects of artificial black pine plantations: analysis of Italian regional laws." Forest@ - Rivista di Selvicoltura ed Ecologia Forestale 15, no. 1 (December 31, 2018): 99–111. http://dx.doi.org/10.3832/efor2985-015.

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36

Nam, Jeongsoo, Keonwoong Lee, Sunjung Park, Hwanil Huh, and Jaye Koo. "Spray Characteristics of a Movable Pintle Injector with Pintle Tip Shape." Journal of the Korean Society for Aeronautical & Space Sciences 47, no. 9 (September 30, 2019): 658–64. http://dx.doi.org/10.5139/jksas.2019.47.9.658.

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37

Ren, Zhao Xu, and Rui Wu. "Effect of Thickness of Pinhole Array on Viewing Angle of Integral Imaging Display." Applied Mechanics and Materials 701-702 (December 2014): 603–6. http://dx.doi.org/10.4028/www.scientific.net/amm.701-702.603.

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A parameter design of a pinhole array is one of the most important keys to design an integral imaging (II) display using pinhole array. The relationship between the thickness of the pinhole array and the viewing angle of the II display is studied, and the maximal value of the thickness is also obtained. When the thickness of the pinhole array is greater than the maximal value, the viewing angle of the II display is decreased with increasing the thickness of the pinhole array. A prototype of the II display using pinhole array is developed, and the experimental results agree well with the theory.
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38

Yan, Qing Song, Zi Peng Tu, Gang Lu, Bai Ping Lu, Chang Chun Cai, and Shou Yin Zhang. "Effect of Vacuum Degree on Pinhole of Vacuum Counter-Pressure Casting Molten Aluminum Alloy." Applied Mechanics and Materials 278-280 (January 2013): 381–84. http://dx.doi.org/10.4028/www.scientific.net/amm.278-280.381.

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During vacuum counter-pressure casting, the vacuumization is an important stage for thin-wall and complicated aluminum alloy castings. Through testing and an analyzing numbers of pinhole and pinhole grade of aluminum alloy samples under different vacuum degree, the effect of vacuum degree on pinhole of vacuum counter- pressure casting molten aluminum alloy is studied. The results indicate vacuum degree has greater effect on pinhole of molten aluminum alloy in vacuumizing process. The smaller vacuum degree is, the more numbers of pinhole of the samples are, and the higher pinhole grade of the samples is. Therefore, when vacuum degree is small, pinhole of molten aluminum alloy appears easily. So the vacuum degree doesn’t choose too small, but for thin-wall and complicated aluminum alloy castings, the vacuum degree doesn’t choose too big either. Appropriate vacuum degree is from 20 KPa to 40 KPa.
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39

Park, Hong Hyun, In Ki Park, Nam Ju Moon, and Yeoun Sook Chun. "Clinical feasibility of pinhole glasses in presbyopia." European Journal of Ophthalmology 29, no. 2 (November 21, 2018): 133–40. http://dx.doi.org/10.1177/1120672118810999.

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Purpose: To investigate the ocular physiologic changes and subjective symptoms of wearing multiple-pinhole glasses in subjects with presbyopia. Methods: This prospective study included 32 eligible subjects with presbyopia. Objective ocular functions and a survey of ocular discomfort were performed at baseline. All participants underwent the same examinations after reading while wearing the pinhole glasses and not wearing these glasses at a 1-week interval in random order. Results: The pinhole glasses improved uncorrected distance and near visual acuity in presbyopia. These glasses also required 15% less accommodative power over the near stimulus of 25 cm than did eyes without pinholes. Compared to reading without pinhole glasses, reading with pinhole glasses led to the following changes: increase in monocular near point of accommodation from 4.39 ± 0.78 diopter (D) to 5.19 ± 1.12 D, increase in depth of focus from 1.42 ± 0.44 D to 2.00 ± 0.33 D, and increase in amplitude of fusional convergence from 13.38 ± 6.88 prism D to 21.62 ± 10.00 prism D. In contrast, the reading speed decreased, inter-blink interval increased, tear break-up time shortened, and subjective ophthalmic symptoms worsened with pinhole glasses compared to without. Conclusion: In presbyopia, pinhole glasses improve visual acuity and accommodation-related parameters by pseudo-accommodation and the pinhole effect. However, the low legibility, increased inter-blink interval, and shortened break-up time of pinhole glasses cause an uncomfortable feeling and excessive eye fatigue. Pinhole glasses have strengths and limitations that must be considered to provide appropriate guidance in patients with presbyopia. Clinical trial registration was done at www.ClinicalTrials.gov (identifier: NCT02722291).
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40

Stovtiz, Steven. "PPE Pinhole Vision Tip." Physician and Sportsmedicine 28, no. 7 (July 2000): 19. http://dx.doi.org/10.3810/psm.2000.07.1093.

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41

Hariharan, P., and M. Roy. "Improved pinhole spatial filter." Optics & Laser Technology 39, no. 1 (February 2007): 155–56. http://dx.doi.org/10.1016/j.optlastec.2005.04.002.

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42

Smith, N. "Classic Project: Pinhole Camera." Engineering & Technology 13, no. 2 (March 1, 2018): 92–93. http://dx.doi.org/10.1049/et.2018.0233.

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43

Bissonnette, D., P. Rochon, and P. Somers. "The complementary pinhole camera." Physics Teacher 29, no. 4 (April 1991): 214. http://dx.doi.org/10.1119/1.2343283.

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44

Jakovidis, Greg. "A pinhole imaging experiment." Physics Teacher 31, no. 8 (November 1993): 500. http://dx.doi.org/10.1119/1.2343854.

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45

Kolner, Brian H. "The pinhole time camera." Journal of the Optical Society of America A 14, no. 12 (December 1, 1997): 3349. http://dx.doi.org/10.1364/josaa.14.003349.

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46

ROBERTS, LES. "Integration at Pingle School." Journal of the Institute of Mental Subnormality (APEX) 8, no. 2 (August 26, 2009): 53–55. http://dx.doi.org/10.1111/j.1468-3156.1980.tb00516.x.

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47

Dawson-Howe, Kenneth M., and David Vernon. "Simple pinhole camera calibration." International Journal of Imaging Systems and Technology 5, no. 1 (1994): 1–6. http://dx.doi.org/10.1002/ima.1850050102.

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48

O'brien, S. B. G. "Asymptotics of a Pinhole." Journal of Colloid and Interface Science 191, no. 2 (July 1997): 514–16. http://dx.doi.org/10.1006/jcis.1997.4982.

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49

Wang, Zhenglin, and William Guo. "Coded pinhole lens imaging." OSA Continuum 1, no. 1 (September 12, 2018): 64. http://dx.doi.org/10.1364/osac.1.000064.

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50

Vega, Andres, Sina Saravi, Thomas Pertsch, and Frank Setzpfandt. "Pinhole quantum ghost imaging." Applied Physics Letters 117, no. 9 (August 31, 2020): 094003. http://dx.doi.org/10.1063/5.0012477.

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