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1

Smith, Russell. "Light Path." Journal of Early Modern Studies 8, no. 2 (2019): 43–79. http://dx.doi.org/10.5840/jems20198212.

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This paper focuses on the mathematisation of mechanics in the seventeenth century, specifically on how the representation of compounded rectilinear motions presented in the ancient Greek Mechanica found its way into Newton’s Principia almost two thousand years later. I aim to show that the path from the former to the latter was optical: the conceptualisation of geometrical lines as paths of reflection created a physical interpretation of dia­grammatic principles of geometrical point-motion, involving the kinematics and dynamics of light reflection. Upon the atomistic conception of light, the o
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2

Usubamatov, Ryspek. "Physics of Gyroscope’s “Antigravity Effect”." Advances in Mathematical Physics 2019 (December 20, 2019): 1–7. http://dx.doi.org/10.1155/2019/4197863.

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The physics of gyroscopic effects are more complex than presented in existing mathematical models. The effects presented by these models do not match the real forces acting on gyroscopic devices. New research in this area has demonstrated that a system of inertial torques, which are generated by the rotating mass of spinning objects, acts upon a gyroscope. The actions of the system of inertial forces are validated by practical tests of the motions of a gyroscope with one side support. The action of external load torque on a gyroscope with one side support demonstrates that the gyroscope’s upwa
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3

Ramzan, Siti Hajar. "Crafting Linear Motion Problems for Problem- Based Learning Physics Classes." International Journal of Psychosocial Rehabilitation 24, no. 5 (2020): 5426–37. http://dx.doi.org/10.37200/ijpr/v24i5/pr2020249.

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4

Chen, Yilin, and Jack W. Baker. "Spatial Correlations in CyberShake Physics‐Based Ground‐Motion Simulations." Bulletin of the Seismological Society of America 109, no. 6 (2019): 2447–58. http://dx.doi.org/10.1785/0120190065.

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Abstract When studying the performance of distributed infrastructure in earthquakes, spatial variations in strong ground motion have a significant impact. Currently, prediction models for spatial ground‐motion variations in future earthquakes are calibrated using ground‐motion observations from densely recorded earthquakes. Although useful, that calibration process requires strong assumptions about stationarity and isotropy of correlations. This article reports results from conducting analogous spatial variation estimation using physics‐based simulations from the CyberShake platform. This plat
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5

Szuromi, P. D. "APPLIED PHYSICS: Canceling Brownian Motion." Science 307, no. 5716 (2005): 1695a. http://dx.doi.org/10.1126/science.307.5716.1695a.

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6

Alvargonzález, David. "Herminio: sculpture, physics and motion." Sculpture Journal 22, no. 1 (2013): 117–32. http://dx.doi.org/10.3828/sj.2013.8.

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7

Henry, John. "Hobbes, Galileo, and the Physics of Simple Circular Motions." Hobbes Studies 29, no. 1 (2016): 9–38. http://dx.doi.org/10.1163/18750257-02901002.

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Hobbes tried to develop a strict version of the mechanical philosophy, in which all physical phenomena were explained only in terms of bodies in motion, and the only forces allowed were forces of collision or impact. This ambition puts Hobbes into a select group of original thinkers, alongside Galileo, Isaac Beeckman, and Descartes. No other early modern thinkers developed a strict version of the mechanical philosophy (not even Newton who allowed forces of attraction and repulsion operating at a distance). Natural philosophies relying solely on bodies in motion require a concept of inertial mo
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8

Drozdek, Adam. "Continuous Motion in Physics VIII 8." Acta Antiqua Academiae Scientiarum Hungaricae 43, no. 1-2 (2003): 59–65. http://dx.doi.org/10.1556/aant.43.2003.1-2.6.

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9

Parmentier, Jan C. "The Physics of Labyrinthine Motion Stimulus." Neurologic Clinics 8, no. 2 (1990): 261–68. http://dx.doi.org/10.1016/s0733-8619(18)30354-2.

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10

Pei, Xiong-Skiba. "Using Interactive Physics in planetary motion." Physics Teacher 36, no. 1 (1998): 42–43. http://dx.doi.org/10.1119/1.879975.

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11

Bracikowski, Christopher, Doug Bowman, Karen Brown, and Russ Madara. "Feeling the physics of linear motion." Physics Teacher 36, no. 4 (1998): 242–43. http://dx.doi.org/10.1119/1.880053.

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12

Chan, Johnny C. L. "THE PHYSICS OF TROPICAL CYCLONE MOTION." Annual Review of Fluid Mechanics 37, no. 1 (2005): 99–128. http://dx.doi.org/10.1146/annurev.fluid.37.061903.175702.

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13

Koupil, Jan, and Vladimír Vícha. "Simple phenomena, slow motion, surprising physics." Physics Education 46, no. 4 (2011): 454–60. http://dx.doi.org/10.1088/0031-9120/46/4/015.

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14

de la Torre, Christopher A., Brendon A. Bradley, and Robin L. Lee. "Modeling nonlinear site effects in physics-based ground motion simulations of the 2010–2011 Canterbury earthquake sequence." Earthquake Spectra 36, no. 2 (2020): 856–79. http://dx.doi.org/10.1177/8755293019891729.

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This study examines the performance of nonlinear total stress one-dimensional (1D) wave propagation site response analysis for modeling site effects in physics-based ground motion simulations of the 2010–2011 Canterbury, New Zealand earthquake sequence. This approach explicitly models three-dimensional (3D) ground motion phenomena at the regional scale, and detailed site effects at the local scale. The approach is compared with a more commonly used empirical VS30-based method of computing site amplification for simulated ground motions, as well as prediction via an empirical ground motion mode
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15

Kahveci̇, Derya, and Yusuf Yayli. "Persistent rigid-body motions on slant helices." International Journal of Geometric Methods in Modern Physics 16, no. 12 (2019): 1950193. http://dx.doi.org/10.1142/s0219887819501937.

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This paper reviews the persistent rigid-body motions and examines the geometric conditions of the persistence of some special frame motions on a slant helix. Unlike the Frenet–Serret motion on general helices, the Frenet–Serret motion on slant helices can be persistent. Moreover, even the adapted frame motion on slant helices can be persistent. This paper begins by explaining one-dimensional rigid-body motions and persistent motions. Then, it continues to present persistent frame motions in terms of their instantaneous twists and axode surfaces. Accordingly, the persistence of any frame motion
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16

BOHM, A., L. J. BOYA, P. KIELANOWSKI, M. KMIECIK, M. LOEWE, and P. MAGNOLLAY. "THEORY OF RELATIVISTIC EXTENDED OBJECTS." International Journal of Modern Physics A 03, no. 05 (1988): 1103–21. http://dx.doi.org/10.1142/s0217751x88000473.

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Physical ideas and mathematical methods of molecular and nuclear physics are extended into the relativistic domain. The resulting models are noncanonical modifications of restricted modes of the string. They describe collective motions of relativistic extended objects in terms of variables which are derived from the symmetry group (for the center-of-mass motion) and from the spectrum generating group (for the intrinsic motion). The simplest relativistic model of this kind is used to calculate spectrum and radiative transitions of hadrons.
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17

Song, Seok Goo, Mathieu Causse, and Jeff Bayless. "Sensitivity Analysis of the Interfrequency Correlation of Synthetic Ground Motions to Pseudodynamic Source Models." Seismological Research Letters 92, no. 1 (2020): 301–13. http://dx.doi.org/10.1785/0220200181.

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Abstract Given the deficiency of recorded strong ground-motion data, it is important to understand the effects of earthquake rupture processes on near-source ground-motion characteristics and to develop physics-based ground-motion simulation methods for advanced seismic hazard assessments. Recently, the interfrequency correlation of ground motions has become an important element of ground-motion predictions. We investigate the effect of pseudodynamic source models on the interfrequency correlation of ground motions by simulating a number of ground-motion waveforms for the 1994 Northridge, Cali
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18

LoLordo, Antonia. "Epicurean and Galilean Motion in Gassendi's Physics." Philosophy Compass 3, no. 2 (2008): 301–14. http://dx.doi.org/10.1111/j.1747-9991.2007.00127.x.

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19

Lincoln, James. "Enhancing physics demos using iPhone slow motion." Physics Teacher 55, no. 9 (2017): 588–89. http://dx.doi.org/10.1119/1.5011847.

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20

Hasnawi, Ahmad. "The Definition of Motion in Avicenna's Physics." Arabic Sciences and Philosophy 11, no. 2 (2001): 219–55. http://dx.doi.org/10.1017/s0957423901001102.

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A part of chapter 1, Book II of the Physics of the šif¯' is dedicated to the aristotelian definition of motion (Physics III, 1, 201a10-11). The developments to which the treatment of this question gives rise are distinctive of the Avicennian style in his Physics. By assuming the notion of double entelechy, Avicenna is following the most classical exegetical tradition. However, by setting a correspondence between the double entelechy and the double notion of motion: 1) motion as an intermediary state, which can be ascribed to a moving object at any instant of its trajectory, and 2) motion as a
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21

Nugraha, Dewanta Arya, C. Cari, A. Suparmi, and Widha Sunarno. "Physics students’ answer on simple harmonic motion." Journal of Physics: Conference Series 1153 (February 2019): 012151. http://dx.doi.org/10.1088/1742-6596/1153/1/012151.

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22

Huggins, Elisha. "Beginning Introductory Physics with Two-Dimensional Motion." Physics Teacher 47, no. 4 (2009): 212–15. http://dx.doi.org/10.1119/1.3098204.

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23

Garcia, Simon, Edouard Hannezo, Jens Elgeti, Jean-François Joanny, Pascal Silberzan, and Nir S. Gov. "Physics of active jamming during collective cellular motion in a monolayer." Proceedings of the National Academy of Sciences 112, no. 50 (2015): 15314–19. http://dx.doi.org/10.1073/pnas.1510973112.

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Although collective cell motion plays an important role, for example during wound healing, embryogenesis, or cancer progression, the fundamental rules governing this motion are still not well understood, in particular at high cell density. We study here the motion of human bronchial epithelial cells within a monolayer, over long times. We observe that, as the monolayer ages, the cells slow down monotonously, while the velocity correlation length first increases as the cells slow down but eventually decreases at the slowest motions. By comparing experiments, analytic model, and detailed particl
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24

Xiao, Boxiang, Sheng Wu, and Xinyu Guo. "A physics-based approach to motion capture data processing for virtual plant modeling and simulation." International Journal of Modeling, Simulation, and Scientific Computing 09, no. 03 (2018): 1840005. http://dx.doi.org/10.1142/s1793962318400056.

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Dynamic virtual plant simulation is an attractive research issue in both botany and computer graphics. Data-driven method is an efficient way for motion analysis and animation synthesis. As a widely used tool, motion capture has been used in plant motion data acquisition and analysis. The most prominent and important problem in motion capture for plants is primary data processing such as missing markers reconstruction. This paper presents a novel physics-based approach to motion capture data processing of plants. Firstly, a physics-based mechanics model is found by Lagrangian mechanics for a m
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25

Corcilius, Klaus, and Pavel Gregoric. "Aristotle’s Model of Animal Motion." Phronesis 58, no. 1 (2013): 52–97. http://dx.doi.org/10.1163/15685284-12341242.

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Abstract In this paper we argue that Aristotle operates with a particular theoretical model in his explanation of animal locomotion, what we call the ‘centralized incoming and outgoing motions’ (CIOM) model. We show how the model accommodates more complex cases of animal motion and how it allows Aristotle to preserve the intuition that animals are self-movers, without jeopardizing his arguments for the eternity of motion and the necessary existence of one eternal unmoved mover in Physics VIII. The CIOM model helps to elucidate Aristotle’s two central yet problematic claims, namely that the sou
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26

Zade, Allan. "Philosophy, physics and mathematics of relative and absolute motion." International Journal of Physical Research 4, no. 2 (2016): 27. http://dx.doi.org/10.14419/ijpr.v4i2.6234.

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The idea of motion includes propagation of signals in a given medium and motion of a physical bodies (including observers) relative to the same medium. Combinations of various types of motion lead to many phenomena detectable and hidden from the observer’s point of view.Usually, light offers the most mysterious way of motion regarding the observer. To reveal the truth and eliminate the mystery, we need to use another sophisticated way of imagination and experimentation to reach a clear view on the fundamental processes of motion despite all illusions, old ideas and wrong postulates.
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27

Luo, A. C. J., and D. O'Connor. "Impacting chatter and stick in a transmission system with two oscillators." Proceedings of the Institution of Mechanical Engineers, Part K: Journal of Multi-body Dynamics 223, no. 3 (2009): 159–88. http://dx.doi.org/10.1243/14644193jmbd202.

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In this article, an investigation on non-linear dynamical behaviours of a transmission system with a gear pair is conducted. The transmission system is described through an impact model with a possible stick between the two gears. From the theory of discontinuous dynamical systems, the motion mechanism of impacting chatter with stick is investigated. The onset and vanishing conditions for stick motions are developed, and the condition for maintaining stick motion is obtained as well. The corresponding physical interpretation is given for a better understanding of non-linear behaviours of gear
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28

Hariwangsa Panuluh, Albertus, Elisabeth Dian Atmajati, and Yosep Dwi Kristanto. "Physics education students’ perception on the use of motion detector in linear motion practicum." Journal of Physics: Conference Series 1470 (February 2020): 012087. http://dx.doi.org/10.1088/1742-6596/1470/1/012087.

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29

Vicovaro, Michele, Stefano Noventa, and Luca Battaglini. "Intuitive physics of gravitational motion as shown by perceptual judgment and prediction-motion tasks." Acta Psychologica 194 (March 2019): 51–62. http://dx.doi.org/10.1016/j.actpsy.2019.02.001.

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30

Thomson, Ethan M., Robin L. Lee, and Brendon A. Bradley. "Ground motion simulations of Hope fault earthquakes." Bulletin of the New Zealand Society for Earthquake Engineering 52, no. 4 (2019): 152–71. http://dx.doi.org/10.5459/bnzsee.52.4.152-171.

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This paper examines ground motions for a major potential Mw7.51 rupture of the Hope Fault using a physics based simulation methodology and a 3D crustal velocity model of New Zealand. The simulation methodology was validated for use in the region through comparison with observations for a suite of historic small magnitude earthquakes located proximal to the Hope Fault. Simulations are compared with conventionally utilised empirical ground motion models, with simulated peak ground velocities being notably higher in regions with modelled sedimentary basins. A sensitivity analysis was undertaken w
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31

Hasegawa, Shoichi, Hironori Mitake, and Yuichi Tazaki. "Springhead: A Physics Engine for Motion and Behavior." Journal of the Robotics Society of Japan 30, no. 9 (2012): 841–48. http://dx.doi.org/10.7210/jrsj.30.841.

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32

WEI, Yi, Shi-Hong XIA, and Zhao-Qi WANG. "Physics-Based Simulation of Human Motion in Flight." Journal of Software 19, no. 12 (2009): 3228–36. http://dx.doi.org/10.3724/sp.j.1001.2008.03228.

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33

Voulodimos, Athanasios, Ioannis Rallis, and Nikolaos Doulamis. "Physics-based keyframe selection for human motion summarization." Multimedia Tools and Applications 79, no. 5-6 (2018): 3243–59. http://dx.doi.org/10.1007/s11042-018-6935-z.

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34

Pomerantsev, A. "Biomechanics, physics and energy modelling of motion control." Journal of Physics: Conference Series 1614 (August 2020): 012092. http://dx.doi.org/10.1088/1742-6596/1614/1/012092.

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35

Rosen, Jacob. "Motion and Change in Aristotle’s Physics 5. 1." Phronesis 57, no. 1 (2012): 63–99. http://dx.doi.org/10.1163/156852812x607298.

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Abstract This paper illustrates how Aristotle’s topological theses about change in Physics 5-6 can help address metaphysical issues. Two distinctions from Physics 5. 1 are discussed: changing per se versus changing per aliud; motion versus change. Change from white to black is motion and alteration, whereas change from white to not white is neither. But is not every change from white to black identical with a change from white to not white? Theses from Physics 6 refute the identity. Is change from white to black at least accompanied by change from white to not white? Perhaps, but given further
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36

Ogborn, Jon, and Edwin F. Taylor. "Quantum physics explains Newton’s laws of motion." Physics Education 40, no. 1 (2004): 26–34. http://dx.doi.org/10.1088/0031-9120/40/1/001.

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37

Muhayyuddin, Aliakbar Akbari, and Jan Rosell. "Physics-based Motion Planning with Temporal Logic Specifications." IFAC-PapersOnLine 50, no. 1 (2017): 8993–99. http://dx.doi.org/10.1016/j.ifacol.2017.08.1578.

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38

Candela, Antonia. "Time and space: undergraduate Mexican physics in motion." Cultural Studies of Science Education 5, no. 3 (2010): 701–27. http://dx.doi.org/10.1007/s11422-010-9259-5.

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39

Kerzel, Dirk. "Representational Momentum Beyond Internalized Physics." Current Directions in Psychological Science 14, no. 4 (2005): 180–84. http://dx.doi.org/10.1111/j.0963-7214.2005.00360.x.

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Prediction of future motion is necessary in order to successfully deal with moving objects. Implicit measures have been used to evaluate the sources of information used in this task. For instance, observers may be asked to localize the final position of a moving target. Judgments have been found to be displaced in the direction of motion (forward displacement), suggesting that observers have internalized a mental analogue of physical momentum. However, more recent studies have shown that forward displacement may not be caused by cognitive mechanisms alone. Rather, predictive mechanisms at the
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40

Conte, Robert, and Laurent de Seze. "Exact solution of the planar motion of three arbitrary point vortices." Modern Physics Letters B 29, no. 35n36 (2015): 1530017. http://dx.doi.org/10.1142/s0217984915300173.

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We give an exact quantitative solution for the motion of three vortices of any strength, which Poincaré showed to be integrable. The absolute motion of one vortex is generally biperiodic: in uniformly rotating axes, the motion is periodic. There are two kinds of relative equilibrium configuration: two equilateral triangles and one or three colinear configurations, their stability conditions split the strengths space into three domains in which the sets of trajectories are topologically distinct. According to the values of the strengths and the initial positions, all the possible motions are cl
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41

Dong, Ran, Dongsheng Cai, and Soichiro Ikuno. "Motion Capture Data Analysis in the Instantaneous Frequency-Domain Using Hilbert-Huang Transform." Sensors 20, no. 22 (2020): 6534. http://dx.doi.org/10.3390/s20226534.

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Motion capture data are widely used in different research fields such as medical, entertainment, and industry. However, most motion researches using motion capture data are carried out in the time-domain. To understand human motion complexities, it is necessary to analyze motion data in the frequency-domain. In this paper, to analyze human motions, we present a framework to transform motions into the instantaneous frequency-domain using the Hilbert-Huang transform (HHT). The empirical mode decomposition (EMD) that is a part of HHT decomposes nonstationary and nonlinear signals captured from th
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42

NAM, SOON-KWON, and KI-BUM KIM. "Stability of an electron beam in a two-frequency wiggler with a self-generated field." Journal of Plasma Physics 77, no. 2 (2010): 257–63. http://dx.doi.org/10.1017/s0022377810000206.

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AbstractWe investigate the relativistic electron motions in a two-frequency wiggler magnetic field with self-generated fields. The equations of motion are derived from the Hamiltonian which include the self-generated field, and we find the steady-state orbit from the equations of motion. The stability of electron motion in a two-frequency wiggler is examined by the numerical simulation. We analyze the a dynamical systems using the fast Fourier transformation and the Poincarè surface of section to find the critical value which have the periodical electron motion and to optimize the two-frequenc
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43

Georgiou, I. T., and I. B. Schwartz. "Slaving the In-Plane Motions of a Nonlinear Plate to Its Flexural Motions: An Invariant Manifold Approach." Journal of Applied Mechanics 64, no. 1 (1997): 175–82. http://dx.doi.org/10.1115/1.2787270.

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We show that the in-plane motions of a nonlinear isotropic plate can be decoupled from its transverse motions. We demonstrate this decoupling by showing analytically and numerically the existence of a global nonlinear invariant manifold in the phase space of three nonlinearly coupled fundamental oscillators describing the amplitudes of the coupled fundamental modes. The invariant manifold carries a continuum of slow periodic motions. In particular, for any motion on the slow invariant manifold, the transverse oscillator executes a periodic motion and it slaves the in-plane oscillators into per
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44

Bauer, Dominique. "Dry friction: from impending motion to motion." Physics Education 29, no. 4 (1994): 239–41. http://dx.doi.org/10.1088/0031-9120/29/4/010.

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45

Grable‐Wallace, Lisa, Joyce Mahoney, and Prabha Ramakrishnan. "Suggested courseware for the non‐calculus physics student: Simple harmonic motion, wave motion, and sound." Physics Teacher 27, no. 2 (1989): 102–5. http://dx.doi.org/10.1119/1.2342679.

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46

Okada, Isao. "MD-Simulation of Molten (Li, K)Cl at the Eutectic Composition. Self-Exchange Velocities of Li- and K-Isotopes near the Cl--Ions." Zeitschrift für Naturforschung A 42, no. 1 (1987): 21–28. http://dx.doi.org/10.1515/zna-1987-0105.

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Molecular dynamics simulation (MD) has been done for a molten (Li, K)Cl mixture of the eutectic composition at about 700 K, 950 K and 1100 K and, for comparison, also for pure LiCl and KCl at about 950 K and 1100 K The atomic masses of half the Li+ and K+ ions have been set at 6.941 and 39.098, respectively. Self-exchange velocities (SEV’s) of these cations have been calculated. The Chemla effect is reflected by the SEV’s. The isotope effects of the SEV’s in the mixture increase slightly with temperature. The motions of the cations with respect to the adjacent CI- are classified into four mode
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47

Vicsek, Tamás, and Anna Zafeiris. "Collective motion." Physics Reports 517, no. 3-4 (2012): 71–140. http://dx.doi.org/10.1016/j.physrep.2012.03.004.

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48

Levi, Federico. "Chilling motion." Nature Physics 15, no. 2 (2019): 110. http://dx.doi.org/10.1038/s41567-019-0431-x.

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49

Zumofen, G., and J. Klafter. "From Dispersion to Laminarity in Dynamical Systems." Zeitschrift für Naturforschung A 49, no. 12 (1994): 1241–47. http://dx.doi.org/10.1515/zna-1994-1225.

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Abstract We study transport in dynamical systems characterized by intermittent chaotic behavior with coexistence of dispersive motion due to periods of localization, and of enhanced diffusion due to periods of laminar motion. This transport is discussed within the continuous-time random walk approach which applies to both dispersive and enhanced motions. We analyze the coexistence for the standard map and for a one-dimensional map.
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50

Yusuf, Akhmad, Ishafit Ishafit, and Toni Kus Indratno. "Amusement Park Physics in Panggon Lunjak (Trampoline): Analysis of Kinematics and Energy Use Video Tracking." International Journal of Science and Applied Science: Conference Series 2, no. 1 (2017): 32. http://dx.doi.org/10.20961/ijsascs.v2i1.16672.

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<p class="Abstract"><em>Panggon Lunjak</em> (trampoline) is one of the famous amusement parks among the people that we can use as a recreation to enjoy a pleasant sensation. Without us knowing the amusement park that we often encounter is actually the result of the application of science and technology, especially in the field of physics, because it is amusement park for student of science is a real laboratory or the giant laboratory that we can use as a study of physics concepts and as research materials. <em>Panggon Lunjak</em> (trampoline) motion is very close
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