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Автор: Grafiati
Опубліковано: 30 травня 2022
Оновлено: 31 травня 2022

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Статті в журналах з теми "Three-dimensional mode"

1

Williamson, C. H. K. "Three-dimensional wake transition." Journal of Fluid Mechanics 328 (December 10, 1996): 345–407. http://dx.doi.org/10.1017/s0022112096008750.

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It is now well-known that the wake transition regime for a circular cylinder involves two modes of small-scale three-dimensional instability (modes A and B), depending on the regime of Reynolds number (Re), although almost no understanding of the physical origins of these instabilities, or indeed their effects on near-wake formation, have hitherto been made clear. We address these questions in this paper. In particular, it is found that the two different modes A and B scale on different physical features of the flow. Mode A has a larger spanwise wavelength of around 3–4 diameters, and scales on the larger physical structure in the flow, namely the primary vortex core. The wavelength for mode A is shown to be the result of an ‘elliptic instability’ in the nearwake vortex cores. The subsequent nonlinear growth of vortex loops is due to a feedback from one vortex to the next, involving spanwise-periodic deformation of core vorticity, which is then subject to streamwise stretching in the braid regios. This mode gives an out-of-phase streamwise vortex pattern.In contrast, mode-B instability has a distinctly smaller wavelength (1 diameter) which scales on the smaller physical structure in the flow, the braid shear layer. It is a manifestation of an instability in a region of hyperbolic flow. It is quite distinct from other shear flows, in that it depends on the reverse flow of the bluff-body wake; the presence of a fully formed streamwise vortex system, brought upstream from a previous half-cycle, in proximity to the newly evolving braid shear layer, leads to an in-phase stream-wise vortex array, in strong analogy with the ‘Mode 1’ of Meiburg & Lasheras (1988) for a forced unseparated wake. In mode B, we also observe amalgamation of streamwise vortices from a previous braid with like-sign vortices in the subsequent braid.It is deduced that the large scatter in previous measurements concerning mode A is due to the presence of vortex dislocations. Dislocations are triggered at the sites of some vortex loops of mode A, and represent a natural breakdown of the periodicity of mode A instability. By minimizing or avoiding the dislocations which occur from end contamination or which occur during wake transition, we find an excellent agreement of both critical Re and spanwise wavelength of mode A with the recent secondary stability analysis of Barkley & Henderson (1996).Wake transition is further characterized by velocity and pressure measurements. It is consistent that, when mode-A instability and large-scale dislocations appear, one finds a reduction of base suction, a reduction of (two-dimensional) Reynolds stress level, a growth in size of the formation region, and a corresponding drop in Strouhal frequency. Finally, the present work leads us to a new clarification of the possible flow states through transition. Right through this regime of Re, there exist two distinct and continuous Strouhal frequency curves: the upper one corresponds with purley small- scale instabilities (e.g. denoted as mode A), while the lower curve corresponds with a combination of small-scale plus dislocation structures (e.g. mode A*). However, some of the flow states are transient or ‘unstable’, and the natural transitioning wake appears to follow the scenario: (2D→A*→B).
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2

Xu, Li Zhong, Jin Liang Li, and Ya Jun Li. "The Three-Dimensional Dynamics for Toroidal Drive." Advanced Materials Research 562-564 (August 2012): 536–39. http://dx.doi.org/10.4028/www.scientific.net/amr.562-564.536.

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In this paper, a model to simulate the dynamic behavior of the toroidal drive is developed. The three-dimensional dynamic model includes all six rigid body motions of the stator, worm, rotor and the planets. Using the model, the natural frequencies and vibration modes of the drive system are investigated. The vibration modes are classified into single modes and coupled modes. The single modes include planet mode, worm mode and stator mode. The vibration and frequency characteristics of different modes are obtained. The relation between modes and half cone angle of the planet tooth is discussed. The relation between vibrations and bearing stiffness is also discussed. When the bearing stiffness is about 10 times of the mesh stiffness, some vibration displacements of the drive system are quite small and can be neglected. Meanwhile, the dynamic equations for the drive system can be simplified.
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3

Kato, K., K. Hokkirigawa, T. Kayaba, and Y. Endo. "Three Dimensional Shape Effect on Abrasive Wear." Journal of Tribology 108, no. 3 (July 1, 1986): 346–49. http://dx.doi.org/10.1115/1.3261193.

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The three dimensional shape effect of asperity on abrasive wear was investigated with in-situ experiments in the scanning electron microscope. The geometry of model asperity was represented by attack angle and dihedral angle, where attack angle changed in 0∼90 deg and dihedral angle in 0∼180 deg. Wear modes of shearing, cutting, and wedge forming were observed and each mode was related to attack angle and dihedral angle by wear mode diagram. Wear rate in cutting mode increased with attack angle and was maximum at a certain dihedral angle.
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4

Brissaud, M., L. Eyraud, and H. Kleimann. "Three‐dimensional model for piezoelectric ceramic mode vibration determination." Journal of the Acoustical Society of America 79, S1 (May 1986): S46. http://dx.doi.org/10.1121/1.2023239.

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5

Xu, Fei, Yu Long Li, and Wan Lin Guo. "Fracture Parameters on Three-Dimensional Sliding Mode Fracture." Key Engineering Materials 340-341 (June 2007): 447–52. http://dx.doi.org/10.4028/www.scientific.net/kem.340-341.447.

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Анотація:
In the recent years three-dimensional (3D) elastic-plastic analyses have been conducted extensively for the opening mode (mode I) fracture and the constraint effects are discussed in detail. However less work is focused on other modes as sliding mode (mode II), tearing mode (mode III) or the mixed mode fracture in three-dimensional. In this paper the thickness effect on pure mode II case is discussed by the finite element method (FEM). Modified Boundary Layer (MBL) model is used, which has the ability to take into account the combined effects of the in-plane constraint (T-stress) and the out-of-plane constraint (finite thickness). The result demonstrates the weak thickness dependence on the near tip stress and strain fields under mode II loading. And the size of the 3D zone at mode II loading is determined to range from 1.0 to 1.2 times the thickness. Two fracture parameters of J integral and crack tip sliding displacement (CTSD) are discussed, which are almost same at different thickness planes except those very near the surface. It is interesting to find that the relations between J and CTSD keep linear at different thickness planes. T-stress is symmetry on stress and strain distributions along the crack plane. However its effects indicate weak thickness dependent on the CTSD and J integral fracture parameter.
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6

Corke, T. C., J. D. Krull, and M. Ghassemi. "Three-dimensional-mode resonance in far wakes." Journal of Fluid Mechanics 239, no. -1 (June 1992): 99. http://dx.doi.org/10.1017/s0022112092004348.

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7

Jiangli Dong, Kin Seng Chiang, and Wei Jin. "Compact Three-Dimensional Polymer Waveguide Mode Multiplexer." Journal of Lightwave Technology 33, no. 22 (November 15, 2015): 4580–88. http://dx.doi.org/10.1109/jlt.2015.2478961.

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8

Luo, WenYu, RenHe Zhang, and Henrik Schmidt. "Three-dimensional mode coupling around a seamount." Science China Physics, Mechanics and Astronomy 54, no. 9 (July 30, 2011): 1561–69. http://dx.doi.org/10.1007/s11433-011-4442-6.

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9

Gao, Huajian. "Three-Dimensional Slightly Nonplanar Cracks." Journal of Applied Mechanics 59, no. 2 (June 1, 1992): 335–43. http://dx.doi.org/10.1115/1.2899525.

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Анотація:
Three-dimensional slightly nonplanar cracks are studied via a perturbation method valid to the first-order accuracy in the deviation of the crack shape from a perfectly planar reference crack. The Bueckner-Rice crack-face weight functions are used in the perturbation analysis to establish a relationship, within first-order accuracy, between the apparent and local stress intensity factors for the nonplanar crack. Perturbation solutions for a cosine wavy crack with arbitrary wavelengths are used to examine the effects of three T-stress components, Txx, TXZ, TZZ, on the stability of a mode 1 planar crack in the x-z plane with front lying along the z-axis. A condition for the mode 1 crack to be stable against three-dimensional wavy perturbations of wavelengths λx and λz is determined as Txx + Tzzg < 0 where g is negative, with a very small magnitude, for 0<λx/λz<1/3 and positive for 1/3<λx/λz<∞; this suggests that when Txx = 0, a compressive stress Tzz may cause crack deflection with large wavelengths parallel to the crack front and a tensile stress Tzz may cause deflection with small wavelengths parallel to the front. For comparable T-stress values, it is shown that a negative Txx always enhances the stability of a mode 1 planar crack and a negative Tzz ensures the stability of a mode 1 crack against perturbations parallel to the crack front. The shear component Txz, while not affecting the mode 1 path stability, induces a mode 3 stress intensity factor once crack deflection occurs, and thus promotes the formation of en echelon-type cracking patterns.
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10

Machida, Kenji. "Three-Dimensional Stress Analysis by Three-dimensional Local Hybrid Method." Key Engineering Materials 306-308 (March 2006): 523–28. http://dx.doi.org/10.4028/www.scientific.net/kem.306-308.523.

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In the displacement measurement inside a specimen by speckle photography, it is not easy to get clear Young's fringes images. Stress-intensity factors of mixed mode can be estimated by embedded speckle photography. However, the error of the stress intensity factor inside a specimen was considerably large. To evaluate the 3-D stress field inside the specimen from displacement data on the free surface obtained from the 2-D intelligent hybrid method, we developed the 3-D local hybrid method based on an inverse problem analysis. The accuracy of the 3-D local hybrid method varies depending on the depth of the plane of error assessment, hybrid domain size, and specimen thickness. Hence the optimal analysis conditions were discussed.
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Дисертації з теми "Three-dimensional mode"

1

Dawes, J. H. P. "Mode interactions in three-dimensional convection." Thesis, University of Cambridge, 2001. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.598414.

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The focus of this thesis is the influence of rotation or a magnetic field on the dynamics of pattern formation by thermal convection in a plane layer (the Rayleigh-Bénard problem). Chapter 1 of the thesis provides a short introduction to the theory of equivalent steady-state and Hopf bifurcations on doubly-periodic lattices in the plane. Known results and new observations for Hopf bifurcations on non-rotating and rotating square lattices are summarised. There is also a detailed presentation of new stability results for the Hopf bifurcation on a square superlattice. In Chapter 2 the effect on convection of an imposed vertical magnetic field is discussed. This leads to a detailed analysis of the simplest three-dimensional Hopf/steady-state mode interaction, where the ratio of the critical wavenumbers for oscillatory and steady convection is 1 : √2. Chapters 3, 4 and 5 contain results on pattern selection in rotating Rayleigh-Bénard convection, specifically for low Prandtl number fields. Calculations in the regime where the onset of convection is oscillatory are performed to determine possible forms of convection at onset. The transition (with increasing Prandtl number) from patterns involving oscillatory rolls to those involving steady rolls is influenced by a second 1 : √2 mode interaction. The resulting amplitude equations contain heteroclinic cycles and bursting behaviour in marked contrast to the magnetoconvection case. Finally, a new asymptotic regime of low Prandtl number and rapid rotation is explored. The relevance of this regime to various sets of experimental results is discussed.
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2

Ogawa, Hiroyuki. "Testing the accuracy of a three-dimensional acoustic coupled mode model." Thesis, Monterey, California. Naval Postgraduate School, 1991. http://hdl.handle.net/10945/26806.

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3

Kosker, Sadik. "Three Dimensional Mixed Mode Fracture Analysis Of Functionally Graded Materials." Master's thesis, METU, 2007. http://etd.lib.metu.edu.tr/upload/12608795/index.pdf.

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The main objective of this study is to model and analyze a three dimensional inclined semi-elliptic surface crack in a Functionally Graded Material (FGM) coating bonded to a homogeneous substrate with a bond coat. The parametric analyses on FGMs are based upon zirconia-yttria (ZrO2-8wt%-Y2O3) FGM coating bonded to a substrate made of a nickel-based superalloy. It is assumed that there is a nickel-chromium&
#8211
aluminum&
#8211
zirconium (NiCrAlY) bond coat between the FGM coating and substrate. Metal-rich, linear variation, ceramic-rich and homogeneous ceramic FGM coating types are considered in the analyses. The inclined semi-elliptic surface crack problem in the FGM coating-bond coat-substrate system is analyzed under transient thermal loading. This problem is modeled and analyzed by utilizing three dimensional finite elements. Strain singularity around the crack front is simulated using collapsed 20 &
#8211
node quarter &
#8211
point brick elements. Three &
#8211
dimensional displacement correlation technique is utilized to extract the mixed mode stress intensity factors around the crack front for different inclination angles of the semi-elliptic surface crack. The energy release rates around the crack front are also calculated by using the evaluated mixed mode stress intensity factors. The results obtained in this study are the peak values of mixed mode stress intensity factors and energy release rates around the crack front for various inclination angles of the semi-elliptic surface crack embedded in the FGM coating of the composite structure subjected to transient thermal loading.
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4

潤, 土田, and Jun Tsuchida. "Dimensional reduction method for three-mode three-way data based on canonical covariance analysis." Thesis, https://doors.doshisha.ac.jp/opac/opac_link/bibid/BB13056385/?lang=0, 2018. https://doors.doshisha.ac.jp/opac/opac_link/bibid/BB13056385/?lang=0.

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3相3元データとは，対象，変量，条件の3つの有限集合組によって表現されるデータの総称であり，マーケティングリサーチ，心理学，経済学などの様々な分野で観測されるデータである．本論文では，多変量解析手法の一つである正準共分散分析を3相3元データに拡張し，その適用例および既存手法との比較を行った．
Three-mode three-way data exist in various research areas, such as psychology and marketing research. We propose new dimensional reduction methods for three-mode three-way data based on canonical covariance analysis in this study. In addition, we include a simulation study and apply the proposed method to real data.
博士(文化情報学)
Doctor of Culture and Information Science
同志社大学
Doshisha University
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5

Gneiting, Scott Alexander. "Improved Leaky-Mode Waveguide Spatial Light Modulators for Three Dimensional Displays." BYU ScholarsArchive, 2017. https://scholarsarchive.byu.edu/etd/6561.

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This thesis improves on the design of the leaky-mode spatial light modulator, LMW-SLM, presented by Dr. Smalley[1]. Improvements include: input coupling gratings, a pulsed laser input, output coupling gratings, and a 3D printed adjustable module for the stabilization of critical alignments. First, input coupling gratings reduce the cost of the LMW-SLM from $500 to around $2, a drop in cost of over two orders of magnitude. This enables multiple modulators to be used in a single display and allows for an inexpensive modular design to be created. Second, a pulsed laser input allows for image creation without the use of a polygon for derotation. Removal of the polygon allows for direct viewing of the LMW-SLM output enabling near-eye and flat panel displays. Third, output coupling gratings allow for bottom exit devices that are essential for thin substrates and flat panel displays. Fourth, the 3D printed module allows for the critical alignments of the LMW-SLM to become permanent. This in turns allows for transportation of the created displays without a trained technician by abstracting away the complexities of the device. The resulting changes simplify hardware, reduce cost, and enable the LMW-SLM to be modularized and the resulting 3D displays to be transportable. These improvements are made possible by the addition of a one new mask step during fabrication, a simple circuit design, and a 3D printed module designed in SOLIDWORKS. Included in this thesis as attachments are the MATLab, Eagle, and SOLIDWORKS files used to create the improved LMW-SLM.
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6

Finlayson, Eric F. "Stress Intensity Factor Distributions in Bimaterial Systems - A Three Dimensional Photoelastic Investigation." Thesis, Virginia Tech, 1998. http://hdl.handle.net/10919/36504.

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Stress-freezing photoelastic experiments are conducted using two different sets of photoelastic materials to investigate stress intensity behavior near to and coincident with bimaterial interfaces. Homogeneous, bonded homogeneous, and bonded bimaterial single edge-cracked tension specimens are utilized throughout the investigation for comparative purposes. The first series of tests involves machined cracks obliquely inclined to the direction of far field tensile loading. Mixed-mode stress intensity factors are observed and quantified using a simplified analytical algorithm which makes use of experimentally measured data. In this series of tests, the bimaterial specimens consist of a photoelastic material bonded to the same material containing a moderate quantity of aluminum powder (for elastic stiffening purposes). Moderate yet similar increases in stress intensity factors are observed in bonded homogeneous and bonded bimaterial specimens, suggesting the presence of bondline residual stresses (rather than elastic modulus mismatch) as the primary contributing factor. The second series of tests involves the bonding of mutually translucent photoelastic materials whose elastic module differ by a ratio of approximately four to one. Cracks are placed both near and coincident to the bimaterial interfaces. Mode-mixity and increases in stress intensity are found only in bimaterial specimens whose cracks are placed close to the bondline. Using the materials from the first series of tests it is shown that the increases in these near-bondline experiments are due to thermal mismatch properties (incurred during the stress freezing cycles) rather than mechanical mismatch properties.
Master of Science
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7

Ficici, Ferhan. "Three Dimensional Fracture Analysis Of Fillet Welds." Master's thesis, METU, 2007. http://etd.lib.metu.edu.tr/upload/3/12608351/index.pdf.

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The aim of this study is to model three dimensional surface crack problems in fillet welds. It is assumed that weld material has the same material properties with the sheet metals. The surface crack is considered to occur at two regions
one at the weld root and the other at the weld toe. The surface crack is assumed to have a semi &ndash
elliptical crack front profile. The surface crack problem is analyzed under mechanical loading and the models are built up by three dimensional finite elements. Around the crack front, strain singularity is taken into account by using degenerated 20 &ndash
node quarter &ndash
point solid elements. The main results of this work are the stress intensity factors around the crack front for the test specimen model subjected to axial and bending loads.
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8

Yentsch, Robert J. "Three-Dimensional Shock-Boundary Layer Interactions in Simulations of HIFiRE-1 and HIFiRE-2." The Ohio State University, 2013. http://rave.ohiolink.edu/etdc/view?acc_num=osu1384195671.

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9

Esmen, Ekrem Alp 1977. "Three-dimensional mixed mode linear elastic fracture mechanics analysis using domain interaction integrals." Thesis, Massachusetts Institute of Technology, 2004. http://hdl.handle.net/1721.1/28377.

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Анотація:
Thesis (S.M.)--Massachusetts Institute of Technology, Dept. of Mechanical Engineering, 2004.
Includes bibliographical references (p. 109-111).
Three-dimensional mixed-mode linear elastic fracture mechanics analysis is presented using domain interaction integrals. An out-of-plane sinusoidal crack was analyzed using a commercially available finite element package to extract the stress intensity factors and the J-Integral. The results were then compared with those obtained from crack face relative displacements as a post-processing step. The model has been tested on various geometries and the performance of focused and non-focused meshing algorithms are compared. The behavior of the stress intensity factors under far-field K-load for growing surface roughness in the form of a sinusoidal crack have been modelled as a cosine series.
by Ekrem Alp Esmen.
S.M.
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10

Sagos, George A. "A three-dimensional coupled normal mode model for sound propagation in shallow water with irregular bottom bathymetry." Thesis, Monterey, California. Naval Postgraduate School, 1992. http://hdl.handle.net/10945/24074.

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Книги з теми "Three-dimensional mode"

1

Ogawa, Hiroyuki. Testing the accuracy of a three-dimensional acoustic coupled mode model. Monterey, Calif: Naval Postgraduate School, 1991.

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2

Sagos, George A. A three-dimensional coupled normal mode model for sound propagation in shallow water with irregular bottom bathymetry. Monterey, Calif: Naval Postgraduate School, 1992.

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3

Yuan, Jianren. A coupled normal-mode approach to three-dimensional sound propagation, including elastic effects from ocean bottom sediments. Ann Arbor, MI: UMI, 1993.

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4

Binhlam, Jacqueline M. Examination of three-dimensional (3-D) effects on sound propagation through mesoscale features using 3-D coupled mode theory. Monterey, Calif: Naval Postgraduate School, 1992.

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5

Seddougui, Sharon O. A nonlinear investigation of the stationary mode of instability of the three-dimensional compressible boundary layer due to a rotating disc. Hampton, Va: ICASE, 1989.

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6

Yu, Faxin. Three-dimensional model analysis and processing. Hangzhuou: Zhejiang University Press, 2010.

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7

Yu, Faxin, Hao Luo, Zheming Lu, and Pinghui Wang. Three-Dimensional Model Analysis and Processing. Berlin, Heidelberg: Springer Berlin Heidelberg, 2010. http://dx.doi.org/10.1007/978-3-642-12651-2.

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8

Lepetit, Vincent. Monocular model-based 3D tracking of rigid objects. Boston, MA: NOW Publishers, 2005.

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9

Sampson, R. Mark. Three dimensional visualization of a coastal mesoscale model. Monterey, Calif: Naval Postgraduate School, 1993.

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10

Linton, Harold. Color model environments: Color andlight in three-dimensional form. New York: Van Nostrand Reinhold, 1985.

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Частини книг з теми "Three-dimensional mode"

1

Its, Alexander R., and Victor Yu Novokshenov. "Quasiclassical mode of the three-dimensional wave collapse." In Lecture Notes in Mathematics, 216–29. Berlin, Heidelberg: Springer Berlin Heidelberg, 1986. http://dx.doi.org/10.1007/bfb0076677.

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2

Xu, Fei, Yu Long Li, and Wan Lin Guo. "Fracture Parameters on Three-Dimensional Sliding Mode Fracture." In Engineering Plasticity and Its Applications, 447–52. Stafa: Trans Tech Publications Ltd., 2007. http://dx.doi.org/10.4028/0-87849-433-2.447.

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3

Dong, Hui Ru, Quan Liang Liu, Zhi Guo Zhang, and Yun Xiang Cheng. "Experimental Methods for Three-Dimensional Mixed Mode Fracture." In Experimental Mechanics in Nano and Biotechnology, 923–26. Stafa: Trans Tech Publications Ltd., 2006. http://dx.doi.org/10.4028/0-87849-415-4.923.

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4

Liang, Yanmin, and Yao Wang. "Integration of Information Technology and Three-Dimensional Teaching Mode." In Data Processing Techniques and Applications for Cyber-Physical Systems (DPTA 2019), 1115–21. Singapore: Springer Singapore, 2020. http://dx.doi.org/10.1007/978-981-15-1468-5_130.

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5

Corke, T. C. "Three-Dimensional Mode Resonances in Boundary Layers, Jets and Wakes." In Advances in Soil Science, 136–49. New York, NY: Springer New York, 1990. http://dx.doi.org/10.1007/978-1-4612-3430-2_17.

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6

Nagao, Kazuma. "Response of the Higgs Mode in a Three Dimensional Optical Lattice." In Springer Theses, 53–81. Singapore: Springer Singapore, 2020. http://dx.doi.org/10.1007/978-981-15-7171-8_4.

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7

Chiu, Ching-Sang, James H. Miller, Warren W. Denner, and James F. Lynch. "A Three-Dimensional, Broadband, Coupled Normal-Mode Sound Propagation Modeling Approach." In Full Field Inversion Methods in Ocean and Seismo-Acoustics, 57–62. Dordrecht: Springer Netherlands, 1995. http://dx.doi.org/10.1007/978-94-015-8476-0_10.

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8

Machida, K., and M. Kikuchi. "Crack-Tip Stress Singularity Field of a Mixed-Mode Three-Dimensional Crack." In Computational Mechanics ’95, 2045–50. Berlin, Heidelberg: Springer Berlin Heidelberg, 1995. http://dx.doi.org/10.1007/978-3-642-79654-8_340.

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9

Mele, Donato. "Tissue Harmonic Imaging, Anatomical M-Mode, and Three-Dimensional Imaging in Stress Echocardiography." In Stress Echocardiography, 253–61. Berlin, Heidelberg: Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/978-3-662-05096-5_22.

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Tanabe, R., Y. Ashizawa, and H. Oka. "CMOS Scaling Analysis based on ITRS Roadmap by Three-dimensional Mixed-mode Device Simulation." In Simulation of Semiconductor Processes and Devices 2004, 303–6. Vienna: Springer Vienna, 2004. http://dx.doi.org/10.1007/978-3-7091-0624-2_71.

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Тези доповідей конференцій з теми "Three-dimensional mode"

1

Guo, Chia-Hao, Wei-Ren Siao, and Jung-Ping Liu. "Optical Scanning Holography in the Coherent Mode." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2014. http://dx.doi.org/10.1364/dh.2014.dtu2b.2.

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2

Wallace, J. Kent, Stephanie Rider, Eugene Serabyn, Chris Lindensmith, and Jay Nadeau. "A Common-Mode Architecture for a Digital Holographic Microscope." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2016. http://dx.doi.org/10.1364/dh.2016.dth3f.2.

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3

Zhang, Lingfei, and Thomas J. Naughton. "Introducing the counter mode of operation into optical image encryption." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2019. http://dx.doi.org/10.1364/dh.2019.th3a.20.

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4

Wallace, J. Kent, Eugene Serabyn, Chris Lindensmith, Stephanie Rider, and Jay Nadeau. "A multiwavelength, common-mode architecture for a digital holographic microscope." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2019. http://dx.doi.org/10.1364/dh.2019.w2b.6.

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5

Lin, Yu-Chih, B. Vinoth, Xin-Ji Lai, Han-Yen Tu, and Chau-Jern Cheng. "Integrated dual-mode tomography for unlabeled free-floating single cell imaging." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2018. http://dx.doi.org/10.1364/dh.2018.dw5f.3.

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McClaughlin, S., C. Leach, A. Henrie, B. Haymore, D. E. Smalley, S. Jolly, and V. M. Bove. "Frequency Division of Color for Holovideo Displays using Anisotropic Leaky Mode Couplers." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2015. http://dx.doi.org/10.1364/dh.2015.dm2a.2.

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Dehaeck, Sam, Yannis Tsoumpas, and Pierre Colinet. "Interferometric profiling of transparent objects in zero-fringe mode using 2D Fan Wavelets." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2015. http://dx.doi.org/10.1364/dh.2015.dth3a.4.

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Park, Heewon, Kyung-Il Joo, Min-Kyu Park, Hee-Dong Jeong, and Hak-Rin Kim. "Development of 2D/3D dual mode Light-field Camera using Fast Switchable Micro lens array." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2016. http://dx.doi.org/10.1364/dh.2017.w2a.33.

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Kim, Young Min, Sungwon Choi, Hyunsik Sung, and Sung-Wook Min. "Projection-type real mode integral imaging system using convex mirror array with three-dimensional screen." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2016. http://dx.doi.org/10.1364/dh.2016.dt4d.3.

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Hsu, Fan-Hsi, Chien-Yuan Han, Tai-Nan Guo, Kun-Huang Chen, Ken-Yuh Hsu, and Jing-Heng Chen. "A Novel Method for Recording Polarization-selective Substrate-mode Volume Holograms with a Large Diffraction Angle." In Digital Holography and Three-Dimensional Imaging. Washington, D.C.: OSA, 2016. http://dx.doi.org/10.1364/dh.2016.dw1d.3.

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Звіти організацій з теми "Three-dimensional mode"

1

Ballard, Megan S. Acoustic Modeling Using a Three-Dimensional Coupled-Mode Model. Fort Belvoir, VA: Defense Technical Information Center, September 2013. http://dx.doi.org/10.21236/ada598885.

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Ballard, Megan S. Acoustic Modeling Using a Three-Dimensional Coupled-Mode Model. Fort Belvoir, VA: Defense Technical Information Center, September 2012. http://dx.doi.org/10.21236/ada574801.

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Ballard, Megan S. Development and Application of a Three-dimensional Seismo-acoustic Coupled-mode Model. Fort Belvoir, VA: Defense Technical Information Center, September 2014. http://dx.doi.org/10.21236/ada617651.

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Sugama, H., and W. Horton. L-H confinement mode dynamics in three-dimensional state space. Office of Scientific and Technical Information (OSTI), January 1994. http://dx.doi.org/10.2172/10126086.

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R. L. Dewar, P. Cuthbert, and R. Ball. Strong ''Quantum'' Chaos in the Global Ballooning Mode Spectrum of Three-dimensional Plasmas. Office of Scientific and Technical Information (OSTI), November 2000. http://dx.doi.org/10.2172/768847.

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Lee, S. Y. Three-Dimensional CFD FLYGT Mixer Model and Results. Office of Scientific and Technical Information (OSTI), April 2002. http://dx.doi.org/10.2172/799718.

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Aviles, B. N. Dynamic Three-Dimensional Process Water Density Model for Ultrasim. Office of Scientific and Technical Information (OSTI), March 2001. http://dx.doi.org/10.2172/781034.

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Russell, H. A. J., A. F. Bajc, A. Burt, C. Logan, R. Muligan, and D. R. Sharpe. A three dimensional surficial stratigraphic model for southern Ontario. Natural Resources Canada/ESS/Scientific and Technical Publishing Services, 2016. http://dx.doi.org/10.4095/297739.

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Cerco, Carl F., Mark R. Noel, and Sung-Chan Kim. Three-Dimensional Eutrophication Model of Lake Washington, Washington State. Fort Belvoir, VA: Defense Technical Information Center, August 2004. http://dx.doi.org/10.21236/ada427041.

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O`Hirok, W. Preliminary results of a three-dimensional radiative transfer model. Office of Scientific and Technical Information (OSTI), September 1995. http://dx.doi.org/10.2172/232601.

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