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Journal articles on the topic 'Blow off'

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Published: 4 June 2021
Last updated: 5 February 2022

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1

Norris, Thomas R. "Fluid blow‐off muffler." Journal of the Acoustical Society of America 91, no. 4 (April 1992): 2302. http://dx.doi.org/10.1121/1.403639.

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2

Norris, Thomas R. "Fluid blow‐off‐muffler." Journal of the Acoustical Society of America 80, no. 4 (October 1986): 1281. http://dx.doi.org/10.1121/1.394456.

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3

Schultze, V., and M. Wagner. "Blow-off of aluminium films." Applied Physics A Solids and Surfaces 53, no. 3 (September 1991): 241–48. http://dx.doi.org/10.1007/bf00324259.

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4

Lovejoy, Thomas E. "Will Expectedly the Top Blow off?" BioScience 45 (January 1995): S3—S6. http://dx.doi.org/10.2307/1312436.

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5

Gent, A. N., and L. H. Lewandowski. "Blow-off pressures for adhering layers." Journal of Applied Polymer Science 33, no. 5 (April 1987): 1567–77. http://dx.doi.org/10.1002/app.1987.070330512.

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6

Barber, J. P., and I. R. McNab. "Magnetic blow-off in armature transition." IEEE Transactions on Magnetics 39, no. 1 (January 2003): 42–46. http://dx.doi.org/10.1109/tmag.2002.805855.

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7

Okuda, Takayoshi, and Hiroyuki Adachi. "Interaction of Laser Blow-Off Blob with a Low-Pressure Gas Discharge." Japanese Journal of Applied Physics 28, Part 2, No. 6 (June 20, 1989): L1055—L1057. http://dx.doi.org/10.1143/jjap.28.l1055.

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8

Bakos, J. S., I. B. Földes, P. N. Ignácz, M. Á. Kedves, and J. Szigeti. "Radiation imprisonment in laser blow-off plasma." Laser and Particle Beams 10, no. 4 (December 1992): 715–21. http://dx.doi.org/10.1017/s0263034600004651.

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Sodium laser blow-off plasma of low temperature (in the 1-eV range) is generated by laser intensities of 108–5.109 W cm−2. Imprisonment of resonant laser light has been observed. These experiments show that basic processes of interaction of radiation with level populations can be studied in the visible range, where the atomic levels have longer lifetimes than the ionic ones in hot plasmas, corresponding to X-ray generation. The imprisonment and resonant effects with various experimental parameters were investigated together with the nonresonant scattering on fragments.
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9

Russell, Daniel H. "Just Blow It Off Because It’s Apocrine?" International Journal of Surgical Pathology 28, no. 4 (September 8, 2019): 412–14. http://dx.doi.org/10.1177/1066896919873070.

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10

Yuan, Ruoyang, James Kariuki, and Epaminondas Mastorakos. "Measurements in swirling spray flames at blow-off." International Journal of Spray and Combustion Dynamics 10, no. 3 (March 23, 2018): 185–210. http://dx.doi.org/10.1177/1756827718763559.

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Various characteristics of swirling spray flames of ethanol, n-heptane, n-decane, and n-dodecane have been measured at conditions far from and close to blow-off using phase Doppler anemometry and OH* chemiluminescence, OH-planar laser-induced fluorescence, and Mie scattering at 5 kHz. The blow-off transient has also been examined. The OH* showed that the two main heat release regions lie around the spray jet at the inner recirculation zone and along the outer shear layer between the inner recirculation zone and the annular air jet. The heat release region is shortened and more attached as the flame approached blow-off. Mie images and phase Doppler anemometry data showed a wider dispersion of the ethanol spray compared to the other fuels. Similar spatial distributions of the Sauter mean diameter were observed for the four fuels for identical flow conditions, with the Sauter mean diameter value increasing with decreasing fuel volatility, but with the exception of significant presence of droplets in the nominally hollow cone for the ethanol spray. The OH-planar laser-induced fluorescence measurements showed an intermittent lift-off from the corner of the bluff body and the average lift-off height decreased with increasing air velocity, with less extinction along the inner flame branch especially for the heavier fuels. At the blow-off conditions, local extinctions appeared at both flame branches. The blow-off process followed a gradual reduction of the size of the flame, with the less volatile fuels showing a more severe flame area reduction compared to the condition far from blow-off. The average blow-off duration, [Formula: see text], calculated from the evolution of the area-integrated OH* signal, was a few tens of milliseconds and for all conditions investigated the ratio [Formula: see text] /( D/ UB) was around 11, but with large scatter. The measurements provide useful information for validation of combustion models focusing on local and global extinction.
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11

Lovejoy, T. E. "AIBS News: Will unexpectedly the top blow off?" BioScience 38, no. 10 (November 1, 1988): 722–26. http://dx.doi.org/10.1093/bioscience/38.10.722.

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12

Tingley, Morgan W., Lyndon D. Estes, and David S. Wilcove. "Climate change must not blow conservation off course." Nature 500, no. 7462 (August 2013): 271–72. http://dx.doi.org/10.1038/500271a.

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13

Zhu, Guoqing, Yunji Gao, Guoqiang Chai, Jinju Zhou, and Shuai Gao. "Experimental study of the width effects on self-induced buoyant blow off in upward flame spread over thin fabric fuels." Textile Research Journal 90, no. 11-12 (November 6, 2019): 1404–13. http://dx.doi.org/10.1177/0040517519886072.

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In this paper, a series of upward flame spreading experiments were conducted on thin flax fabric with various widths ranging from 3.0 to 8.0 cm and length of 1.6 m. Symmetric ignition at the entire bottom edge of samples led to two-sided upward flame growth initially. A very interesting behavior of flame blown off was observed in upward flame spreading and an explanation was provided based on the increased buoyancy-induced velocity at the flame base. When the sample width is 6 cm or less, the flame length increases to a critical value and, correspondingly, the buoyancy-induced velocity reaches the blow off velocity, which results in a flame being blown off on one side. The remaining flame on the other side would shrink in length and propagate to the end of the sample with an asymptotically constant length and steady spread rate. For samples wider than 6 cm, the two-sided flame continues to spread to the end of samples and the self-induced blow off phenomenon is not observed. Moreover, the width effects on the flame height, flame thickness and flame spread rate are analyzed and explained in this paper. The results of this study may help advance better understanding of flame blow off behaviors over solid surfaces and have implications concerning fire control of flame spread over solid fuels.
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14

Jia, Senqing, Fusheng Wang, Weichao Huang, and Bin Xu. "Research on the Blow-Off Impulse Effect of a Composite Reinforced Panel Subjected to Lightning Strike." Applied Sciences 9, no. 6 (March 19, 2019): 1168. http://dx.doi.org/10.3390/app9061168.

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The blow-off impulse effect of a composite reinforced panel subjected to lightning strike is studied combing electric-thermal coupling with explicit dynamic methods. A finite element model of a composite reinforced panel is established under the action of 2.6/10.5 µs impulse current waveform with current peak 60 kA. Blow-off impulse elements are selected according to numerical results of electric-thermal coupling analysis. Elements failure, pressure, and von Mises stress distribution are discussed when blow-off impulse analysis is completed. The results show that the blow-off impulse effect can alter the damage forms of a composite reinforced panel and causes the damage distribution to deviate from the initial fiber direction in each layer. Elements failure modes around the blow-off impulse area are similar to that around the attachment area of the lightning strike. The blow-off impulse effect can well model the internal damage, concave pit, and bulge phenomenon around the attachment area. Additionally, pressure contours are not presented as an anisotropic characteristic but an isotropic characteristic under the blow-off impulse effect, which indicates that the mechanical behavior of composite materials presents as an anisotropic characteristic in low pressure while as an isotropic characteristic in high pressure. This method is suitable to evaluate shock damage of a composite reinforced panel induced by lightning strike.
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15

Umyshev, Dias, Abay Dostiyarov, Andrey Kibarin, Galya Tyutebayeva, Gaziza Katranova, and Darkhan Akpanbetov. "Experimental investigation of distance between v-gutters on flame stabilization and NOx emissions." Thermal Science 23, no. 5 Part B (2019): 2971–81. http://dx.doi.org/10.2298/tsci180503007u.

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Blow-off performance and NOx emissions of the propane and air mixture in a rectangular combustion chamber with bluff bodies were investigated experimentally and numerically. The effects of distance between bluff bodies on NOx emissions, the blow-off limit, and exhaust gas temperature were examined. It was observed that NOx emissions are highly dependent on distance between V-gutters. The re-circulation zone behind the bluff body expands in width based on the decrease of distance between V-gutters, and expands in length with the increase of inlet velocity. The temperature fields behind the bluff body show a similar change, the temperature behind the bluff body reaches its highest when the distance between V-gutters reaches 20 mm, meaning it has better flame stability. The blow-off limit is significantly improved with the decrease of distance between V-gutters. The blow-off limit is greatly improved by reducing the distance between the V-gutters. Maximum blow-off limit of 0.11 is reached in the case of 20 mm, compared with 0.16 at 50 mm at a speed of 10 m/s.
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16

Sasaki, Satoshi, Shuichi Takamura, and Kiyoshi Kadota. "Numerical analysis on laser blow-off lithium beam probing." Kakuyūgō kenkyū 62, no. 4 (1989): 282–95. http://dx.doi.org/10.1585/jspf1958.62.282.

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17

IWAMOTO, Tetsuya, Makoto IKEDA, Takamitsu YOSHIMOTO, and Toshimi TAKAGI. "Lifting/Blow-off and Behaviors of the Diffusion Flame." Proceedings of Conference of Kansai Branch 2002.77 (2002): _5–37_—_5–38_. http://dx.doi.org/10.1299/jsmekansai.2002.77._5-37_.

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18

Bakos, J. S., G. Burger, I. B. Foldes, P. E. Giese, P. N. Ignacz, G. Petravich, J. Szigeti, and S. Zoletnik. "Edge plasma density measurement by laser blow-off method." Plasma Physics and Controlled Fusion 31, no. 5 (May 1, 1989): 693–98. http://dx.doi.org/10.1088/0741-3335/31/5/002.

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19

Bakos, J. S., P. N. Ignácz, J. Szigeti, and J. Kovács. "Laser blow‐off plasma propagating in low‐pressure gas." Applied Physics Letters 51, no. 10 (September 7, 1987): 734–36. http://dx.doi.org/10.1063/1.98850.

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20

Stoecker, Randy. "Strategies for enhancing learning in the ?blow-off? course." Innovative Higher Education 14, no. 2 (1990): 141–53. http://dx.doi.org/10.1007/bf00889615.

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21

Qiao, Hai Jun, and Dian Rong Gao. "Numerical Simulation and Analysis for Blow-Off Flow Field of a Wet Skin Pass Mill." Applied Mechanics and Materials 597 (July 2014): 238–41. http://dx.doi.org/10.4028/www.scientific.net/amm.597.238.

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Blow-off air nozzles blow away the residual emulsion from roll gap and strip surface. Algorithm SIMPLY were used for the finite element numerical simulation for a representational air nozzle blow-off flow field near the roll gap in a cold-rolled skin pass mill. The working conditions of the blow-off flow field was the combination of gas pressure of 0, 2, 5 and 10bar and flip angle of 0°, 5°, 10°, 15°, 20° and 25°. The study provides a reference for control and optimization for the removal process of residual emulsion and design, manufacture, model selection and optimization for the related air nozzles.
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22

Umyshev, Dias, Abay Dostiyarov, Musagul Tumanov, and Quiwang Wang. "Experimental investigation of V-gutter flameholders." Thermal Science 21, no. 2 (2017): 1011–19. http://dx.doi.org/10.2298/tsci151209072u.

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Combustion characteristics and NOx emissions of propane and air mixture in a channel with a bluff body were investigated experimentally. Effects of the angle and type of the flameholder on the NOx emissions, blow-off limit, combustion efficiency, and exhaust gas temperature were examined. The results show that the NOx emissions are dependent on flameholder type and angle. Also it was observed that the perforated V-gutters considerably increases the blow-off performance. Moreover, the blow-off limit decreases as the geometrical size of flame-holder is increased. In addition, the combustion efficiency increase first and then decrease with the increase of the angle. The physics of the combustion process behind V-gutter flameholdes has been discussed. On the basis of experiment authors presented a modified version of the formula for calculation of lean blow-off limits when using bluff bodies, such as V-gutter flameholders.
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23

Wang, Dengwang, Yong Gao, Wei Chen, Shanghui Yang, Jing Zhang, Jie Wang, and Sheng Wang. "The Blow-Off Impulse Equivalence of Typical Missile Homogeneous Al-Alloy under Multienergy Composite Spectrum Electron Beam and Powerful Pulsed X-ray." Materials 14, no. 17 (September 1, 2021): 5002. http://dx.doi.org/10.3390/ma14175002.

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The electron beam, one of the most effective approaches to simulate the irradiation effects of powerful pulsed X-ray in the laboratory, plays an important role in simulating the thermodynamic effects of powerful pulsed X-ray. This paper studies the thermodynamics equivalence between multienergy composite spectrum electron beam and blackbody spectrum X-ray, which is helpful to quickly determine the experimental parameters in the simulation experiment. The experimental data of electron beam are extrapolated by numerical calculation, to increase the range of energy flux. Through calculating the blow-off impulse of blackbody spectrum X-ray irradiation, we obtained the curve of X-ray blow-off impulse varying with energy flux, and then found two categories of equivalent relations—equal-energy flux and equal-impulse—by analyzing the calculation results of electron beam and X-ray blow-off impulse. Based on such relations, we could directly or indirectly obtain the results of blackbody spectrum X-ray irradiation blow-off impulse via electron beam experiment.
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24

Wang, Dengwang, Yong Gao, Wei Chen, Jing Zhang, and Sheng Wang. "Equivalent Analysis of Thermo-Dynamic Blow-Off Impulse under X-ray Irradiation." Applied Sciences 11, no. 19 (September 23, 2021): 8853. http://dx.doi.org/10.3390/app11198853.

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X-ray thermodynamic effect is an important damage mode for spacecraft. Blow-off impulse as the main thermodynamic damage parameter has been widely studied by combining laboratory and numerical simulations. In this paper, most calculations and analyses have been carried out by using the self-developed software RAMA, including the equivalent calculation of blow-off impulse of monoenergetic and blackbody X-ray, and soft/hard blackbody X-ray irradiated at different incidence angles of LY-12 aluminium target. The results show that the characteristic mono-energetic X-ray can be exploited to simulate the blow-off impulse of the blackbody X-ray under certain conditions as a feasible equivalent method for the equal-flux and equal-impulse relations between mono-energetic and intense pulse blackbody of blow-off impulse. Moreover, the equivalent thermodynamic effect can be achieved between the point source radiation and parallel X-ray of X-ray. Furthermore, the cosine distribution of blow-off impulse is conducive to designing and calculating X-ray radiation load of hard aluminium corresponding to 1–5 keV blackbody spectrum. The mentioned results can be referenced for pulse X-ray simulation source and enhance the fidelity of the thermal-mechanical effect by electron beam. It is noteworthy that the study on the thermodynamic effects of intense pulsed X-ray is of high significance.
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25

Adachi, Hiroyuki, Takeshi Noda, Kumeyo Kishi, and Takayoshi Okuda. "Particle composition of laser blow-off used for impurity study." Kakuyūgō kenkyū 59, no. 2 (1988): 123–30. http://dx.doi.org/10.1585/jspf1958.59.123.

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26

Wagh, Ashvin, Rajnish Nagarkar, Gauri Kokane, Sirshendu Roy, Vijay Palawe, Nayana Kulkarni, and Samadhan Pawar. "Oral malignancy and its fickle blow off: A retrospective study." Journal of Cancer Research and Therapeutics 15, no. 3 (2019): 604. http://dx.doi.org/10.4103/jcrt.jcrt_188_18.

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27

Lammer, H., N. V. Erkaev, P. Odert, K. G. Kislyakova, M. Leitzinger, and M. L. Khodachenko. "Probing the blow-off criteria of hydrogen-rich ‘super-Earths’." Monthly Notices of the Royal Astronomical Society 430, no. 2 (January 29, 2013): 1247–56. http://dx.doi.org/10.1093/mnras/sts705.

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28

Yamaguchi, Shigeki, Norio Ohiwa, and Tatsuya Hasegawa. "Structure and blow-off mechanism of rod-stabilized premixed flame." Combustion and Flame 62, no. 1 (October 1985): 31–41. http://dx.doi.org/10.1016/0010-2180(85)90091-4.

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29

Kocsis, G., J. S. Bakos, and P. N. Ign�cz. "Experimental comparison of blow-off methods for plasma-density measurements." Applied Physics B Photophysics and Laser Chemistry 49, no. 5 (November 1989): 415–18. http://dx.doi.org/10.1007/bf00325342.

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30

Galarneau, Elisabeth, and Terry F. Bidleman. "Modelling the temperature-induced blow-off and blow-on artefacts in filter-sorbent measurements of semivolatile substances." Atmospheric Environment 40, no. 23 (July 2006): 4258–68. http://dx.doi.org/10.1016/j.atmosenv.2006.04.006.

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31

Vance, Faizan Habib, Yuriy Shoshin, Philip de Goey, and Jeroen van Oijen. "Flame Stabilization and Blow-Off of Ultra-Lean H2-Air Premixed Flames." Energies 14, no. 7 (April 2, 2021): 1977. http://dx.doi.org/10.3390/en14071977.

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The manner in which an ultra-lean hydrogen flame stabilizes and blows off is crucial for the understanding and design of safe and efficient combustion devices. In this study, we use experiments and numerical simulations for pure H2-air flames stabilized behind a cylindrical bluff body to reveal the underlying physics that make such flames stable and eventually blow-off. Results from CFD simulations are used to investigate the role of stretch and preferential diffusion after a qualitative validation with experiments. It is found that the flame displacement speed of flames stabilized beyond the lean flammability limit of a flat stretchless flame (ϕ=0.3) can be scaled with a relevant tubular flame displacement speed. This result is crucial as no scaling reference is available for such flames. We also confirm our previous hypothesis regarding lean limit blow-off for flames with a neck formation that such flames are quenched due to excessive local stretching. After extinction at the flame neck, flames with closed flame fronts are found to be stabilized inside a recirculation zone.
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32

KOCSIS, G., J. S. BAKOS, S. KÁLVIN, L. KÖNEN, G. MANK, and A. POSPIESZCZYK. "Toroidal transport studies in TEXTOR using lithium laser blow-off injection." Journal of Plasma Physics 58, no. 1 (July 1997): 19–30. http://dx.doi.org/10.1017/s0022377897005795.

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The toroidal spread of laser blow-off injected lithium is studied. The temporal variation of the toroidal and radial distributions of the first two ionization stages of cross-field-injected lithium is measured around the injection location by a gated, image-intensified CCD camera. Broad atomic distribution and deep radial penetration of the injected beam is observed. The toroidal delay of the arrival of the Li+ ions is investigated by detecting the intensity of their line radiation at different toroidal positions away from the injection port. Possible explanations for the observations and the possible mechanism for the toroidal spread are discussed in detail. A comparison of the detected distribution of Li ions with a 1D simulation is presented.
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33

Derjaguin, B. V., and V. V. Karassev. "Viscosity studies of liquid boundary layers by the blow-off method." Progress in Surface Science 40, no. 1-4 (May 1992): 301–8. http://dx.doi.org/10.1016/0079-6816(92)90056-n.

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34

Kumar, Rajneesh, Ajai Kumar, R. K. Singh, and Jinto Thomas. "Experimental investigation of oscillatory structures in laser-blow-off plasma plume." Physics Letters A 375, no. 20 (May 2011): 2064–70. http://dx.doi.org/10.1016/j.physleta.2011.04.007.

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35

Martins, N., M. G. Carvalho, N. H. Afgan, and A. I. Leontiev. "Experimental verification and calibration of the blow-off heat flux sensor." Applied Thermal Engineering 18, no. 6 (March 1998): 481–89. http://dx.doi.org/10.1016/s1359-4311(97)00044-6.

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36

Kumar, Bhupesh, R. K. Singh, and Ajai Kumar. "Dynamics of laser-blow-off induced Li plume in confined geometry." Physics of Plasmas 20, no. 8 (August 2013): 083511. http://dx.doi.org/10.1063/1.4818900.

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37

Bakos, J. S., I. B. Földes, P. N. Ignácz, and G. Kocsis. "Investigation of laser blow‐off atomic beams by electron impact excitation." Journal of Applied Physics 69, no. 3 (February 1991): 1231–36. http://dx.doi.org/10.1063/1.347308.

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38

Baseman, Robert J., and Nan M. Froberg. "Time‐resolved transmission of thin gold films during laser blow‐off." Applied Physics Letters 55, no. 18 (October 30, 1989): 1841–43. http://dx.doi.org/10.1063/1.102182.

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39

Bakos, J. S., G. Burger, P. N. Ignacz, J. Szigeti, and J. Kovacs. "Measuring set-up for investigation of the laser blow-off processes." Journal of Physics E: Scientific Instruments 21, no. 11 (November 1988): 1095–97. http://dx.doi.org/10.1088/0022-3735/21/11/018.

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40

Narihara, K., and S. Hirokura. "Cleaning of Thomson scattering window by a laser blow‐off method." Review of Scientific Instruments 63, no. 6 (June 1992): 3527–28. http://dx.doi.org/10.1063/1.1143847.

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41

Kypraiou, Anna-Maria, Andrea Giusti, Patton M. Allison, and Epaminondas Mastorakos. "Dynamics of acoustically forced non-premixed flames close to blow-off." Experimental Thermal and Fluid Science 95 (July 2018): 81–87. http://dx.doi.org/10.1016/j.expthermflusci.2018.01.036.

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42

Bakos, J. S., I. B. Földes, P. N. Ignácz, M. Á. Kedves, and J. Szigeti. "Interaction of sodium laser blow-off beam with resonant laser radiation." Optics Communications 83, no. 3-4 (June 1991): 210–14. http://dx.doi.org/10.1016/0030-4018(91)90164-9.

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43

Howley, Kirsten, Robert Managan, and Joseph Wasem. "Blow-off momentum from melt and vapor in nuclear deflection scenarios." Acta Astronautica 103 (October 2014): 376–81. http://dx.doi.org/10.1016/j.actaastro.2014.06.022.

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44

Lu, Yong, Xinyan Huang, Longhua Hu, and Carlos Fernandez-Pello. "Concurrent Flame Spread and Blow-Off Over Horizontal Thin Electrical Wires." Fire Technology 55, no. 1 (October 22, 2018): 193–209. http://dx.doi.org/10.1007/s10694-018-0785-0.

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45

Tyliszczak, Artur, Davide E. Cavaliere, and Epaminondas Mastorakos. "LES/CMC of Blow-off in a Liquid Fueled Swirl Burner." Flow, Turbulence and Combustion 92, no. 1-2 (July 4, 2013): 237–67. http://dx.doi.org/10.1007/s10494-013-9477-5.

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46

Kariuki, James, James R. Dawson, and Epaminondas Mastorakos. "Measurements in turbulent premixed bluff body flames close to blow-off." Combustion and Flame 159, no. 8 (August 2012): 2589–607. http://dx.doi.org/10.1016/j.combustflame.2012.01.005.

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47

Lin, Shaorun, Tsz Him Chow, and Xinyan Huang. "Smoldering propagation and blow-off on consolidated fuel under external airflow." Combustion and Flame 234 (December 2021): 111685. http://dx.doi.org/10.1016/j.combustflame.2021.111685.

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48

Boopathi, S., P. Maran, V. Caleb Eugene, and S. Prabhu. "Analysis of Lift off Height and Blow-Off Mechanism of Turbulent Flame by V-Gutter Bluff Body." Applied Mechanics and Materials 787 (August 2015): 727–31. http://dx.doi.org/10.4028/www.scientific.net/amm.787.727.

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The experimental investigation has been carried out to study the stabilization and blowout mechanisms of turbulent flame stabilized by V-gutter bluff body in a square duct at reactive and non-reactive conditions. V-shaped bluff bodies made of stainless steel having 1.6 mm thicknessare used for stabilization of the flame.Experiments have been conducted at selective velocities of commercially available methane and oxygen with 60 degree V-gutter as flame holder. It is observed that at stoichiometric conditions, the V-gutter is dominated by shear layer stabilized flames. The flame stability is influenced by bluff body dimensions and mass flow rate which play a major role in combustion instabilities mixing of air fuel ratio and blow off. The lift off decreases at higher blockage ratios.A strong recirculation zone is found in this test rig immediately downstream of the V-Gutter which gradually subsides and disappears far downstream.The lift off height is not much affected by the velocity of the fuel-air mixture.
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49

Lee, P. H. Y., and O. Willi. "A model for inhibition of thermal transport in laser produced plasmas." Laser and Particle Beams 3, no. 3 (August 1985): 263–71. http://dx.doi.org/10.1017/s0263034600001476.

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We show that the thermal transport in laser produced plasmas can be inhibited due to the outward plasma blow-off which is in the opposite direction to the inward heat transport. A simple model is proposed in which the steady state heat transfer equation, including the convective term for a point heat source, is solved. A simple analytical expression for the ratio of effective to classical conductivity depending on the blow-off velocity is obtained. With this model, present experimental data on thermal transport can be qualitatively, but consistently described.
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50

Marbach, T. L., and A. K. Agrawal. "Experimental Study of Surface and Interior Combustion Using Composite Porous Inert Media." Journal of Engineering for Gas Turbines and Power 127, no. 2 (April 1, 2005): 307–13. http://dx.doi.org/10.1115/1.1789516.

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Abstract:
Combustion using silicon carbide coated, carbon–carbon composite porous inert media (PIM) was investigated. Two combustion modes, surface and interior, depending upon the location of flame stabilization, were considered. Combustion performance was evaluated by measurements of pressure drop across the PIM, emissions of NOx and CO, and the lean blow-off limit. Data were obtained for the two combustion modes at identical conditions for a range of reactant flowrates, equivalence ratios, and pore sizes of the PIM. Results affirm PIM combustion as an effective method to extend the blow-off limit in lean premixed combustion.
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