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Journal articles on the topic 'Instability and transition'

Author: Grafiati

Published: 6 September 2023

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1

Morkovin, Mark V. "Instability and Transition." International Journal of Heat and Fluid Flow 12, no. 4 (1991): 384. http://dx.doi.org/10.1016/0142-727x(91)90029-u.

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2

Men, Hongyuan, Xinliang Li, and Hongwei Liu. "Direct numerical simulations of hypersonic boundary layer transition over a hypersonic transition research vehicle model lifting body at different angles of attack." Physics of Fluids 35, no. 4 (2023): 044111. http://dx.doi.org/10.1063/5.0146651.

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This paper performs direct numerical simulations of hypersonic boundary layer transition over a Hypersonic Transition Research Vehicle (HyTRV) model lifting body designed by the China Aerodynamic Research and Development Center. Transitions are simulated at four angles of attack: 0°, 3°, 5°, and 7°. The free-stream Mach number is 6, and the unit Reynolds number is 107 m−1. Four distinct transitional regions are identified: the shoulder cross-flow and vortex region and the shoulder vortex region on the leeward side, the windward vortex region and the windward cross-flow region on the windward s

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3

Marshall, Victor W., Philippa J. Clarke, and Peri J. Ballantyne. "Instability in the Retirement Transition." Research on Aging 23, no. 4 (2001): 379–409. http://dx.doi.org/10.1177/0164027501234001.

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4

Dagaut, J., M. E. Negretti, G. Balarac, and C. Brun. "Linear to turbulent Görtler instability transition." Physics of Fluids 33, no. 1 (2021): 014102. http://dx.doi.org/10.1063/5.0033944.

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5

Lee, S. Y., and J. M. Wang. "Microwave Instability across the Transition Energy." IEEE Transactions on Nuclear Science 32, no. 5 (1985): 2323–25. http://dx.doi.org/10.1109/tns.1985.4333900.

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6

COOK, ANDREW W., WILLIAM CABOT, and PAUL L. MILLER. "The mixing transition in RayleighTaylor instability." Journal of Fluid Mechanics 511 (July 25, 2004): 333–62. http://dx.doi.org/10.1017/s0022112004009681.

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7

Bayly, B. J., S. A. Orszag, and T. Herbert. "Instability Mechanisms in Shear-Flow Transition." Annual Review of Fluid Mechanics 20, no. 1 (1988): 359–91. http://dx.doi.org/10.1146/annurev.fl.20.010188.002043.

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8

CHAURASIA, HEMANT K., and MARK C. THOMPSON. "Three-dimensional instabilities in the boundary-layer flow over a long rectangular plate." Journal of Fluid Mechanics 681 (June 16, 2011): 411–33. http://dx.doi.org/10.1017/jfm.2011.205.

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A detailed numerical study of the separating and reattaching flow over a square leading-edge plate is presented, examining the instability modes governing transition from two- to three-dimensional flow. Under the influence of background noise, experiments show that the transition scenario typically is incompletely described by either global stability analysis or the transient growth of dominant optimal perturbation modes. Instead two-dimensional transition effectively can be triggered by the convective Kelvin–Helmholtz (KH) shear-layer instability; although it may be possible that this could b

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9

Granatosky, Michael C., Caleb M. Bryce, Jandy Hanna, et al. "Inter-stride variability triggers gait transitions in mammals and birds." Proceedings of the Royal Society B: Biological Sciences 285, no. 1893 (2018): 20181766. http://dx.doi.org/10.1098/rspb.2018.1766.

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Speed-related gait transitions occur in many animals, but it remains unclear what factors trigger gait changes. While the most widely accepted function of gait transitions is that they reduce locomotor costs, there is no obvious metabolic trigger signalling animals when to switch gaits. An alternative approach suggests that gait transitions serve to reduce locomotor instability. While there is evidence supporting this in humans, similar research has not been conducted in other species. This study explores energetics and stride variability during the walk–run transition in mammals and birds. Ac

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10

Kobayashi, Ryoji. "Review: Laminar-to-Turbulent Transition of Three-Dimensional Boundary Layers on Rotating Bodies." Journal of Fluids Engineering 116, no. 2 (1994): 200–211. http://dx.doi.org/10.1115/1.2910255.

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The laminar-turbulent transition of three-dimensional boundary layers is critically reviewed for some typical axisymmetric bodies rotating in still fluid or in axial flow. The flow structures of the transition regions are visualized. The transition phenomena are driven by the compound of the Tollmien-Schlichting instability, the crossflow instability, and the centrifugal instability. Experimental evidence is provided relating the critical and transition Reynolds numbers, defined in terms of the local velocity and the boundary layer momentum thickness, to the local rotational speed ratio, defin

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11

Loiseau, Jean-Christophe, Jean-Christophe Robinet, Stefania Cherubini, and Emmanuel Leriche. "Investigation of the roughness-induced transition: global stability analyses and direct numerical simulations." Journal of Fluid Mechanics 760 (November 4, 2014): 175–211. http://dx.doi.org/10.1017/jfm.2014.589.

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AbstractThe linear global instability and resulting transition to turbulence induced by an isolated cylindrical roughness element of height $h$ and diameter $d$ immersed within an incompressible boundary layer flow along a flat plate is investigated using the joint application of direct numerical simulations and fully three-dimensional global stability analyses. For the range of parameters investigated, base flow computations show that the roughness element induces a wake composed of a central low-speed region surrounded by a three-dimensional shear layer and a pair of low- and high-speed stre

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12

Kleif, Helle Bendix. "A Typology of Transition Patterns Involving Long-Term NEET Episodes: Accumulation of Risk and Adversity." Youth 3, no. 1 (2023): 170–83. http://dx.doi.org/10.3390/youth3010012.

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This paper uses Danish population-based administrative registers to study contemporary school-to-work transitions among young adults who experience long-term NEET episodes between age 16 and 20. By applying sequence analysis and clustering, this paper identifies five distinct transition patterns. Using this typology as the outcome variable in multinomial regression the paper offers insight into how experiences and circumstances, developing until age 16, can affect the subsequently unfolding transition process. Finally, the paper looks ahead and describes whether transitional difficulty accumul

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13

Hernandez, Rafael, and Konstantin I. Matveev. "Transition to Instability in Segmented Rijke Tube." Open Thermodynamics Journal 4, no. 1 (2009): 141–43. http://dx.doi.org/10.2174/1874396x010040100141.

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14

Tohline, J. E. "Star formation - Phase transition, not Jeans instability." Astrophysical Journal 292 (May 1985): 181. http://dx.doi.org/10.1086/163144.

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15

Williamson, C. H. K. "Mode A secondary instability in wake transition." Physics of Fluids 8, no. 6 (1996): 1680–82. http://dx.doi.org/10.1063/1.868949.

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16

Sharma, Prateek, Gregory W. Hammett, and Eliot Quataert. "Transition from Collisionless to Collisional Magnetorotational Instability." Astrophysical Journal 596, no. 2 (2003): 1121–30. http://dx.doi.org/10.1086/378234.

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17

Fomby, Paula, and Stacey J. Bosick. "Family Instability and the Transition to Adulthood." Journal of Marriage and Family 75, no. 5 (2013): 1266–87. http://dx.doi.org/10.1111/jomf.12063.

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18

Finlay, W. H., J. B. Keller, and J. H. Ferziger. "Instability and transition in curved channel flow." Journal of Fluid Mechanics 194, no. -1 (1988): 417. http://dx.doi.org/10.1017/s0022112088003052.

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19

Freeman, Walter J., and Mark D. Holmes. "Metastability, instability, and state transition in neocortex." Neural Networks 18, no. 5-6 (2005): 497–504. http://dx.doi.org/10.1016/j.neunet.2005.06.014.

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20

YURI, MICHIKO. "Phase transition, non-Gibbsianness and subexponential instability." Ergodic Theory and Dynamical Systems 25, no. 4 (2005): 1325–42. http://dx.doi.org/10.1017/s0143385704000926.

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21

Mohamadou, Alidou, A. Kenfack-Jiotsa, and T. C. Kofané. "Modulational instability and spatiotemporal transition to chaos." Chaos, Solitons & Fractals 27, no. 4 (2006): 914–25. http://dx.doi.org/10.1016/j.chaos.2005.04.039.

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22

Avery, Montie, Cedric Dedina, Aislinn Smith, and Arnd Scheel. "Instability in large bounded domains—branched versus unbranched resonances." Nonlinearity 34, no. 11 (2021): 7916–37. http://dx.doi.org/10.1088/1361-6544/ac2a15.

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Abstract We study transitions from convective to absolute instability near a trivial state in large bounded domains for prototypical model problems in the presence of transport and negative nonlinear feedback. We identify two generic scenarios, depending on the nature of the linear mechanism for instability, which both lead to different, universal bifurcation diagrams. In the first, classical case of a linear branched resonance the transition is hard, that is, small changes in a control parameter lead to a finite-size state. In the second, novel case of an unbranched resonance, the transition

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23

Li, Xiao-guang, Changhong Li, Yuan Li, and Pu-jin Zhang. "Research of Transitional Failure Mode as Damage Evolution in Rock Wall." Advances in Civil Engineering 2020 (September 7, 2020): 1–12. http://dx.doi.org/10.1155/2020/8864074.

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The stress condition of tunnel surrounding rock mass is complex. The stress concentration of in situ brittle rock mass caused by excavation results in localized damage evolution parallel to the free face, which is called surface instability. The rock wall shows the transition characteristics of the failure mode with the distance from the surface to the depth. Low strength surface instability and transition failure modes of the tunnel’s rock wall are common in deep condition but cylindrical specimens cannot simulate stress state of rock wall surface well in conventional rock mechanics tests. Th

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24

Motsay, R. W., K. E. Anderson, and R. P. Behringer. "The onset of convection and turbulence in rectangular layers of normal liquid 4He." Journal of Fluid Mechanics 189 (April 1988): 263–86. http://dx.doi.org/10.1017/s0022112088001004.

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We have carried out high-precision measurements of the heat transport in intermediate-size rectangular layers of convecting normal liquid 4He with Prandtl numbers of 0.52 and 0.70. The containers used for these experiments had horizontal dimensions, in units of the height d, of 13.4 × 5.95 (cell I) and 18.2 × 8.12 (cell II). The slopes N1 of the Nusselt curves were 0.56 and 0.70 respectively for cell I and cell II. These values are significantly lower than predictions for N1 for horizontally unbound layers, but comparable with results obtained in cylindrical containers of liquid helium with ro

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25

Lee, Sang Jin, and Tamer A. Zaki. "Simulations of natural transition in viscoelastic channel flow." Journal of Fluid Mechanics 820 (May 5, 2017): 232–62. http://dx.doi.org/10.1017/jfm.2017.198.

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Orderly, or natural, transition to turbulence in dilute polymeric channel flow is studied using direct numerical simulations of a FENE-P fluid. Three Weissenberg numbers are simulated and contrasted to a reference Newtonian configuration. The computations start from infinitesimally small Tollmien–Schlichting (TS) waves and track the development of the instability from the early linear stages through nonlinear amplification, secondary instability and full breakdown to turbulence. At the lowest elasticity, the primary TS wave is more unstable than the Newtonian counterpart, and its secondary ins

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26

Benedek, András, and Péter Klekner. "Managing Economic Transition." Industry and Higher Education 11, no. 3 (1997): 182–88. http://dx.doi.org/10.1177/095042229701100312.

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In the early stages of economic transition in Hungary, stagnation was the dominant characteristic of the country, accompanied by crisis indicators such as marked internal and especially external economic instability, instability in foreign trade, and structural impediments to development. Massive unemployment, a decrease in real wages, evident even today, and the intensification of social inequalities contributed additional tensions to the initial transition phase. In this paper, the authors first outline the main characteristics of the Hungarian economy. Then, against this background, they di

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27

Lavagno, A. "Nuclear phase transition and thermodynamic instabilities in dense nuclear matter." EPJ Web of Conferences 182 (2018): 03007. http://dx.doi.org/10.1051/epjconf/201818203007.

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We study the presence of thermodynamic instabilities in a nuclear medium at finite temperature and density where nuclear phase transitions can take place. Such a phase transition is characterized by pure hadronic matter with both mechanical instability (fluctuations on the baryon density) that by chemical-diffusive instability (fluctuations on the electric charge concentration). Similarly to the liquid-gas phase transition, the nucleonic and the Δ-matter phase have a different isospin density in the mixed phase. In the liquid-gas phase transition, the process of producing a larger neutron exce

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28

Lenz, Brenda. "The Transition From Adolescence to Young Adulthood: A Theoretical Perspective." Journal of School Nursing 17, no. 6 (2001): 300–306. http://dx.doi.org/10.1177/10598405010170060401.

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Life transitions are periods in time when individuals experience major changes. Transitions may occur during periods between two relatively stable states of human development. The associated changes with the transition bring instability as the person passes through the period. During this period, the individual is typically required to make major adjustments, to develop new skills, or to learn to cope with new experiences. One major life transition begins during the final year or years of high school. This transition, unlike childhood transitions, for many individuals will include a move from

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29

Hendi, Seyed Hossein, Shahram Panahiyan, and Behzad Eslam Panah. "Geometrical Method for Thermal Instability of Nonlinearly Charged BTZ Black Holes." Advances in High Energy Physics 2015 (2015): 1–12. http://dx.doi.org/10.1155/2015/743086.

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We consider three-dimensional BTZ black holes with three models of nonlinear electrodynamics as source. Calculating heat capacity, we study the stability and phase transitions of these black holes. We show that Maxwell, logarithmic, and exponential theories yield only type one phase transition which is related to the root(s) of heat capacity, whereas, for correction form of nonlinear electrodynamics, heat capacity contains two roots and one divergence point. Next, we use geometrical approach for studying classical thermodynamical behavior of the system. We show that Weinhold and Ruppeiner metr

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30

Thurlow, M. S., B. J. Brooks, P. G. J. Lucas, M. R. Ardron, J. K. Bhattacharjee, and A. L. Woodcraft. "Convective instability in rotating liquid 3He-4He mixtures." Journal of Fluid Mechanics 313 (April 25, 1996): 381–407. http://dx.doi.org/10.1017/s002211209600225x.

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Thermal convection is investigated experimentally in a dilute liquid mixture of 3He in 4He at four temperatures between 20 and 100 mK above the superfluid transition temperature, chosen for their proximity to the codimension-two and hydrodynamic tricritical points. Two experimental cells of aspect ratio 2.76 and 1.00 were used. For the cell with the higher aspect ratio, two convective transitions at each of the four temperatures were observed above a critical angular velocity, and only one observed below. At temperatures lower than that of the hydrodynamic tricritical point the transition with

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31

Jia, Lingchun, Hongchun Yuan, Yingli Chang, Mu Gu, and Jiajie Zhu. "Dynamic instability of lithiated phosphorene." RSC Advances 10, no. 53 (2020): 32259–64. http://dx.doi.org/10.1039/d0ra04885b.

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32

Jacob, Niya Mary, and Tiju Thomas. "Nanorod to quantum dot conversion in ZnO dispersions with co-surfactants." RSC Advances 5, no. 20 (2015): 15154–58. http://dx.doi.org/10.1039/c4ra05778c.

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A chemically-induced nanorod to QD transition is achieved using co-surfactants. This is different from the physical instability driven transitions reported so far in nanowires and polymers. We propose a suitable mechanism for the observed phenomenon.

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33

DOU, HUA-SHU, and BOO CHEONG KHOO. "ENERGY SPECTRUM OF DISTURBANCE AT TURBULENT TRANSITION VIA ENERGY GRADIENT METHOD." International Journal of Modern Physics: Conference Series 19 (January 2012): 293–303. http://dx.doi.org/10.1142/s2010194512008884.

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The energy gradient theory for flow instability and turbulent transition was proposed in our previous work. The theoretical result obtained accords well with some experimental data for pipe and channel flows in the literature. In the present study, the energy gradient theory is extended to examine the effect of disturbance frequency on turbulent transition. Then, the energy spectrum of disturbance at the turbulent transition is obtained, which scales with the wave number by an exponent of –2. This scaling is near to the K41 law of –5/3 for the full developed isentropic homogenous turbulence. T

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34

MALIK, MUJEEB R., FEI LI, MEELAN M. CHOUDHARI, and CHAU-LYAN CHANG. "Secondary instability of crossflow vortices and swept-wing boundary-layer transition." Journal of Fluid Mechanics 399 (November 25, 1999): 85–115. http://dx.doi.org/10.1017/s0022112099006291.

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Crossflow instability of a three-dimensional boundary layer is a common cause of transition in swept-wing flows. The boundary-layer flow modified by the presence of finite-amplitude crossflow modes is susceptible to high-frequency secondary instabilities, which are believed to harbinger the onset of transition. The role of secondary instability in transition prediction is theoretically examined for the recent swept-wing experimental data by Reibert et al. (1996). Exploiting the experimental observation that the underlying three-dimensional boundary layer is convectively unstable, non-linear pa

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35

Hatman, A., and T. Wang. "A Prediction Model for Separated-Flow Transition." Journal of Turbomachinery 121, no. 3 (1999): 594–602. http://dx.doi.org/10.1115/1.2841357.

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The present study formulates an improved approach for analyzing separated-flow transition that differentiates between the transition process in boundary layers that are laminar at separation and those that are already transitional at separation. The paper introduces new parameters that are necessary in classifying separated-flow transition modes and in accounting for the concomitant evolution of transition in separated shear layer and the average effect of periodic separation bubble build-up and vortex shedding. At least three separated-flow transition modes are positively distinguished: (a) t

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36

Bharuthram, R., and M. A. Hellberg. "Low-frequency drift-induced instabilities in a magnetized two-ion plasma." Journal of Plasma Physics 35, no. 3 (1986): 393–412. http://dx.doi.org/10.1017/s0022377800011429.

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Numerical solutions of a dispersion relation for low-frequency electrostatic waves in a current-carrying, cold, weakly collisional, magnetized two-ion plasma are used to discuss the two-stream and resistive natures of the ion-ion hybrid instability. An instability with analogous behaviour is found to be associated with the light ion cyclotron frequency. Analytical results explain the behaviour. A numerically derived transition diagram summarizes the parameter values for which transitions between different modes take place.

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37

Ma, Wei. "Investigation of Material Instability Behaviors Caused by Combined Stress Loadings." Key Engineering Materials 535-536 (January 2013): 168–72. http://dx.doi.org/10.4028/www.scientific.net/kem.535-536.168.

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This study involves the stability of plastic flow of thermoviscoplastic materials. The general instability criterion is proposed for determining the onset conditions of instability and the transition conditions among various plastic deformation behaviors. By using the phase diagram method, the transition of material instability modes under complex loading conditions is described and the analytical results are further validated with numerical examples.

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38

Riaz, Syed Shahed, Sandip Kar, and Deb Shankar Ray. "Differential flow induced transition of Hopf instability to Turing instability and pattern formation." Physica D: Nonlinear Phenomena 203, no. 3-4 (2005): 224–32. http://dx.doi.org/10.1016/j.physd.2005.04.003.

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39

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 o

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40

Imayama, Shintaro, P. Henrik Alfredsson, and R. J. Lingwood. "An experimental study of edge effects on rotating-disk transition." Journal of Fluid Mechanics 716 (January 28, 2013): 638–57. http://dx.doi.org/10.1017/jfm.2012.564.

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AbstractThe onset of transition for the rotating-disk flow was identified by Lingwood (J. Fluid. Mech., vol. 299, 1995, pp. 17–33) as being highly reproducible, which motivated her to look for absolute instability of the boundary-layer flow; the flow was found to be locally absolutely unstable above a Reynolds number of 507. Global instability, if associated with laminar–turbulent transition, implies that the onset of transition should be highly repeatable across different experimental facilities. While it has previously been shown that local absolute instability does not necessarily lead to l

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41

EL AKOURY, R., M. BRAZA, R. PERRIN, G. HARRAN, and Y. HOARAU. "The three-dimensional transition in the flow around a rotating cylinder." Journal of Fluid Mechanics 607 (June 30, 2008): 1–11. http://dx.doi.org/10.1017/s0022112008001390.

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The flow around a circular cylinder rotating with a constant angular velocity, placed in a uniform stream, is investigated by means of two- and three-dimensional direct numerical simulations. The successive changes in the flow pattern are studied as a function of the rotation rate. Suppression of vortex shedding occurs as the rotation rate increases (>2). A second kind of instabilty appears for higher rotation speed where a series of counter-clockwise vortices is shed in the upper shear layer. Three-dimensional computations are carried out to analyse the three-dimensional transition under t

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42

BLACKBURN, H. M., and S. J. SHERWIN. "Instability modes and transition of pulsatile stenotic flow: pulse-period dependence." Journal of Fluid Mechanics 573 (February 2007): 57–88. http://dx.doi.org/10.1017/s0022112006003740.

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The instability modes arising within simple non-reversing pulsatile flows in a circular tube with a smooth axisymmetric constriction are examined using global Floquet stability analysis and direct numerical simulation. The sectionally averaged pulsatile flow is represented with one harmonic component superimposed on a time-mean flow. We have previously identified a period-doubling global instability mechanism associated with alternating tilting of the vortex rings that are ejected out of the stenosis throat with each pulse. Here we show that while alternating tilting of vortex rings is the pri

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43

Zhou, Ling, Chao Yan, Zi Hui Hao, and Wei Xuan Kong. "A “Laminar + Transition Criteria” Model for Hypersonic Three-Dimensional Boundary Layer Transition Prediction." Applied Mechanics and Materials 798 (October 2015): 627–31. http://dx.doi.org/10.4028/www.scientific.net/amm.798.627.

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A “laminar + transition criteria” model utilizingReθ/MeandReCFcriteria in conjunction with an intermittency functionΓis developed in this paper. With pretreated computational grid and total enthalpyh0=(h0,∞)maxcriteria the boundary layer edge and crossflow velocity can be obtained by using parallel methodology. Validation is accomplished via HIFiRE-5 and a blunt cone with small angle of attack. Results show that computedReθ/MeandReCFdistributions are similar to theN-factor for streamwise instability and crossflow instability from linear PSE methods. The shape and trend of transition regions pr

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44

Janssen, R. J. A., and R. A. W. M. Henkes. "Influence of Prandtl number on instability mechanisms and transition in a differentially heated square cavity." Journal of Fluid Mechanics 290 (May 10, 1995): 319–44. http://dx.doi.org/10.1017/s0022112095002539.

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The transition from laminar to turbulent of the natural-convection flow inside a square, differentially heated cavity with adiabatic horizontal walls is calculated, using the finite-volume method. The purpose of this study is firstly to determine the dependence of the laminar-turbulent transition on the Prandtl number and secondly to investigate the physical mechanisms responsible for the bifurcations observed. It is found that in the square cavity, for Prandtl numbers between 0.25 and 2.0, the transition occurs through periodic and quasi-periodic flow regimes. One of the bifurcations is relat

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45

Nimura, Tomohiro, and Takahiro Tsukahara. "Viscoelasticity-Induced Instability in Plane Couette Flow at Very Low Reynolds Number." Fluids 7, no. 7 (2022): 241. http://dx.doi.org/10.3390/fluids7070241.

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Elasto-inertial turbulence (EIT), a new turbulent state found in polymer solutions with viscoelastic properties, is associated with drag-reduced turbulence. However, the relationship between EIT and drag-reduced turbulence is not currently well-understood, and it is important to elucidate the mechanism of the transition to EIT. The instability of viscoelastic fluids has been studied in a canonical wall-bounded shear flow to investigate the transition process of EIT. In this study, we numerically deduced that an instability occurs in the linearly stable viscoelastic plane Couette flow for lower

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46

Lavagno, A., D. Pigato, and G. Gervino. "Thermodynamic instabilities in high energy heavy-ion collisions." Modern Physics Letters B 29, no. 18 (2015): 1550092. http://dx.doi.org/10.1142/s021798491550092x.

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One of the very interesting aspects of high energy heavy-ion collisions experiments is a detailed study of the thermodynamical properties of strongly interacting nuclear matter away from the nuclear ground state. In this direction, many efforts were focused on searching for possible phase transitions in such collisions. We investigate thermodynamic instabilities in a hot and dense nuclear medium where a phase transition from nucleonic matter to resonance-dominated [Formula: see text]-matter can take place. Such a phase transition can be characterized by both mechanical instability (fluctuation

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47

Singh, N. K. "Instability and Transition in a Laminar Separation Bubble." Journal of Applied Fluid Mechanics 12, no. 5 (2019): 1511–25. http://dx.doi.org/10.29252/jafm.12.05.29607.

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48

Gorton, Gary, and Andrew Winton. "Banking in Transition Economies: Does Efficiency Require Instability?" Journal of Money, Credit and Banking 30, no. 3 (1998): 621. http://dx.doi.org/10.2307/2601261.

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49

Link, Bennett. "Deflagration instability in the quark-hadron phase transition." Physical Review Letters 68, no. 16 (1992): 2425–28. http://dx.doi.org/10.1103/physrevlett.68.2425.

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Tanaka, Toyoichi, Shao-Tang Sun, Yoshitsugu Hirokawa, et al. "Mechanical instability of gels at the phase transition." Nature 325, no. 6107 (1987): 796–98. http://dx.doi.org/10.1038/325796a0.

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