Bibliografie tematiche / Magnetic pressure

Letteratura scientifica selezionata sul tema "Magnetic pressure"

Autore: Grafiati
Pubblicato: 1 giugno 2024

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Articoli di riviste sul tema "Magnetic pressure":

1

Kuchin, Anatoly, Zdenek Arnold, Jiri Kamarád e Sergey Platonov. "Magnetic properties of Tm2Fe16 under pressure". EPJ Web of Conferences 185 (2018): 04018. http://dx.doi.org/10.1051/epjconf/201818504018.

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The magnetic properties of the non-stoichiometric Tm2Fe16 compound under hydrostatic pressures up to 1 GPa were studied. We have revealed that the high-temperature ferrimagnetic state easily magnetized in the basal plane is very sensitive to the volume changes and even moderate pressure is sufficient to its complete suppression and transformation to a helimagnetic state. At the same time, the low-temperature ferrimagnetic state easily magnetized along the hexagonal axis does not disappear under pressure and the temperature of its transition to the high-temperature magnetic states increases under pressure. The remarkable stability of the ground ferrimagnetic state under external pressure can be attributed to the strengthening of the uniaxial magnetic anisotropy and to the mutual perpendicular orientation of the magnetic moments in the ground and the high-temperature magnetic states.
2

Bacri, J. C., J. Lenglet, R. Perzynski e J. Servais. "Magnetic fluid pressure sensor". Journal of Magnetism and Magnetic Materials 122, n. 1-3 (aprile 1993): 399–402. http://dx.doi.org/10.1016/0304-8853(93)91118-q.

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3

Fisher, Shaun, e George Pickett. "Up the magnetic pressure". Nature 444, n. 7121 (dicembre 2006): 832–33. http://dx.doi.org/10.1038/444832a.

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4

Cornelius, Andrew L., Brant Abeln, Daniel Antonio, Jason Baker, Patricia E. Kalita e Ravhi S. Kumar. "High Pressure Materials Physics Research at UNLV". Materials Science Forum 783-786 (maggio 2014): 1836–38. http://dx.doi.org/10.4028/www.scientific.net/msf.783-786.1836.

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High-pressure studies on strongly correlated-electron systems allow the study of the relationship between structural, elastic, electronic, and magnetic properties of d-and f-band systems. The High Pressure Science and Engineering Center (HiPSEC) at UNLV performs interdisciplinary research on a wide variety of materials at high pressures. One such system, YbB2 displays antiferromagnet order at ambient pressure. We present heat capacity measurements at high magnetic fields to 9 T and structural measurement at pressures up to 5 GPa on YbB2.
5

BÄRNER, K., J. W. SCHÜNEMANN, K. HEINEMANN, A. A. GANIN, Yu S. BERSENEV e I. V. MEDVEDEVA. "CORRELATION OF TRANSPORT AND TOPOLOGICAL/SPIN DISORDER FOR SOME AMORPHOUS METALLIC AND MAGNETIC ALLOYS". International Journal of Modern Physics B 07, n. 01n03 (gennaio 1993): 968–71. http://dx.doi.org/10.1142/s0217979293002109.

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The resistivity ρ and the permeability μ of amorphous magnetic ribbons (Fe100−xMnx)75P15C10 are determined at ambient pressure and pressures up to 15 kbar and correlated with the topological and magnetic disorder. The characterization includes the Curie temperature Tc, its pressure derivative ∂Tc/∂p and the pressure dependence of the resistivity minimum temperature.
6

Tseneklidou, Dimitra, Christos G. Tsagas e John D. Barrow. "Relativistic magnetised perturbations: magnetic pressure versus magnetic tension". Classical and Quantum Gravity 35, n. 12 (16 maggio 2018): 124001. http://dx.doi.org/10.1088/1361-6382/aac07f.

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7

Begunovich, Lyudmila V., Maxim M. Korshunov e Sergey G. Ovchinnikov. "Magnetic Collapse in Fe3Se4 under High Pressure". Materials 15, n. 13 (29 giugno 2022): 4583. http://dx.doi.org/10.3390/ma15134583.

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Electronic structure and magnetic properties of Fe3Se4 are calculated using the density functional approach. Due to the metallic properties, magnetic moments of the iron atoms in two nonequivalent positions in the unit cell are different from ionic values for Fe3+ and Fe2+ and are equal to M1=2.071μB and M2=−2.042μB, making the system ferrimagnetic. The total magnetic moment for the unit cell is 2.135μB. Under isotropic compression, the total magnetic moment decreases non-monotonically and correlates with the non-monotonic dependence of the density of states at the Fermi level N(EF). For 7% compression, the magnetic order changes from the ferrimagnetic to the ferromagnetic. At 14% compression, the magnetic order disappears and the total magnetic moment becomes zero, leaving the system in a paramagnetic state. This compression corresponds to the pressure of 114 GPa. The magnetic ordering changes faster upon application of an isotropic external pressure due to the sizeable anisotropy of the chemical bondings in Fe3Se4. The ferrimagnetic and paramagnetic states occur under pressures of 5.0 and 8.0 GPa, respectively. The system remains in the metallic state for all values of compression.
8

Sokolovskiy, V. V., M. A. Zagrebin e V. D. Buchelnikov. "Magnetocaloric Effect of Mn<sub>2</sub>YSn (Y = Sc, Ti, V) Alloys". Физика металлов и металловедение 124, n. 11 (1 novembre 2023): 1122–28. http://dx.doi.org/10.31857/s0015323023601265.

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Abstract—In this paper, the structural, magnetic, and thermodynamic properties of Mn2YSn (Y = Sc, Ti, and V) alloys are considered depending on the applied pressure using the density functional theory and the Monte Carlo method. It is shown that for each compound there are two magnetic states with a low and a high magnetic moment at a smaller and larger unit cell volume, separated by an energy barrier. The barrier value depends on the applied external pressure. The two phases become almost equal in energy at critical pressures of 3.4, –2.9, and –3.25 GPa for Mn2ScSn, Mn2TiSn, and Mn2VSn, respectively. The temperature behavior of the magnetization and magnetocaloric characteristics for the studied phases at various pressures is obtained. Accounting for pressure leads to an understanding of the mechanism of the increase in the magnetocaloric effect in the phase with a high magnetic moment. The greatest effect (ΔSmag ≈ 0.158 J/mol K and ΔTad ≈ 1.1 K) is predicted for Mn2TiSn at a pressure of –2.9 GPa and a change in the magnetic field from 0 to 2 T.
9

KOMIYA, Kinichi, Ikuo ITOH e Katsunori MITSUNAGA. "Pressure Sensing Using Magnetic Fluid". Transactions of the Society of Instrument and Control Engineers 26, n. 7 (1990): 833–35. http://dx.doi.org/10.9746/sicetr1965.26.833.

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10

Gassmann, Stefan, e Lienhard Pagel. "Magnetic actuated pressure relief valve". Sensors and Actuators A: Physical 194 (maggio 2013): 106–11. http://dx.doi.org/10.1016/j.sna.2012.12.033.

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Ti possono interessare anche gli elenchi estesi di opere sul tema "Magnetic pressure":
Articoli di riviste Tesi Libri

Tesi sul tema "Magnetic pressure":

1

Renshaw, Matthew Peter. "Magnetic resonance studies at elevated temperature and pressure". Thesis, University of Cambridge, 2015. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.709303.

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Ghannadzadeh, Saman. "Investigating magnetism and superconductivity using high magnetic fields". Thesis, University of Oxford, 2014. http://ora.ox.ac.uk/objects/uuid:4b78618e-89a3-424e-a673-59d363a2605d.

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This thesis investigates a number of transition-metal coordination polymers and iron-pnictide superconductors through the use of high magnetic fields, low temperatures, and on occasion, high pressures. The thesis will begin by describing my development of the proximity detector dynamic susceptometer, a novel technique that can be used for magnetometery and transport measurements in high magnetic fields. This technique is highly compact and has no moving parts, making it suitable for use in pressure cells, hence opening the way for a variety of new experiments. Through high-field magnetometery and other measurements, I will demonstrate that the pressure can be used to directly control the magnetic properties of the polymeric magnet CuF2(H2O)2(pyrazine). In particular, I observe a transition from quasi-two-dimensional to quasi-one-dimensional antiferromagnetism at 9~kbar, driven by the rotation of the Jahn-Teller axis. I will then present a series of measurements on two coordination polymers, showing how a small chemical difference can lead to drastically different magnetic properties. I show that [Cu(pyrazine)H2O(glycine)2]ClO4 is an excellent spin-chain, while the sister compound [Cu(pyrazine)(glycine)]ClO4 is a dimerised material that shows a spin-gap and is disordered down to very low temperatures, but then undergoes a field-induced phase transition to an ordered phase. I will also describe a series of pulsed-field measurements of the upper critical field of the iron-based superconductors NaFe1-xCoxAs across the whole of the doping phase diagram. It is shown that paramagnetic pair-breaking effects dominate the critical field when the field is parallel to the crystal planes. In the parent compound the paramagnetic limit is equal to that expected from BCS theory, but becomes significantly enhanced above the BCS limit upon doping. It is shown that the multi-band nature of the superconductivity leads to a convex curvature in the evolution of the critical field as the temperature is reduced.
3

Wensley, Joanne Ruth. "High pressure studies on magnetic metals near quantum critical points". Thesis, University of Cambridge, 2011. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.609926.

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4

Furukawa, Masaru. "Localized pressure-driven MHD instabilities in reversed-magnetic-shear tokamaks". Kyoto University, 2001. http://hdl.handle.net/2433/150492.

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Abstract (sommario):
Kyoto University (京都大学)
0048
新制・課程博士
博士(エネルギー科学)
甲第9045号
エネ博第32号
新制||エネ||9(附属図書館)
UT51-2001-F375
京都大学大学院エネルギー科学研究科エネルギー基礎科学専攻
(主査)教授 若谷 誠宏, 教授 近藤 克己, 教授 佐野 史道
学位規則第4条第1項該当
5

Blaauw, Leopold V. "X-ray Scattering and Absorption and High Pressure Magnetisation Studies of 3d Transition Metal Magnetic Compounds and the Development of High Pressure Magnetic Compton Scattering". Thesis, University of Warwick, 2007. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.490685.

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Magnetic Compton scattering was performed on the weak itinerant ferromagnet MnSi providing a direct measurement of the one dimensional spin-dependent electron momentum density of the sample. These results were then compared to band structure calculations performed by the Bristol positron group. The complementary technique of X-ray magnetic circular dichroism was utilised to measure the spin to orbital magnetic moment ratio of NiO nanoparticles. High pressure magnetisation studies were performed on the rare Earth perovskite EUO.5SSr0.42Mn03 and led to the construction of a new ambient and high pressure magnetic phase diagram. The technique of magnetic Compton scattering has been extended into the high pressure regime via the use of a diamond anvil cell capable ofpressures ofup to 20 GPa. The rare Earth perovskite EU0.5SSr0.42Mn03 exhibits a large magnetic moment in the ferromagnetic metal phase. The phase diagram proposed by previous authors was reanalysed in the light of new magnetometry data. A SQUID clamp cell was used to extend the study of the new phase diagram into the high pressure regime. Behaviour which is indicative of. the formation of ferromagnetic clusters within an antiferromagnetic matrix is observed at low temperatures and fields. The application of pressure radically suppresses antiferromagnetism with the sample and favours ferromagnetic ordering via the double exchange mechanism. A new high pressure phase diagram is proposed. The intermetallic compound MnSi exhibits weak ferromagnetism below a temperature of 29K under an applied field of 0.6T. Band structure calculations, when compared to experimentally obtained magnetic Compton profiles fail to adequately explain· the observed momentum densities for pz < 2 a.u. However, the features observed in the profiles at higher momentum are described well by the LMTO theory. The discrepancies at low momentum are the result of the incorrect weighting of the d-like bands. The spin moment was measured as 0.36 ± 0.005 J.lB f.u.-1 indicating a 10% orbital contribution to the total observed moment of 0.4 J.lB f.u.-I A study ofNiO nanoparticles revealed a critical surface to volume ratio which results in a large enhancement of the ferromagnetisation. X-ray absorption spectra indicate that this enhancement is due to the formation of a thicker surface layer of Ni2+ spin symmetry and that the contribution to the spectra from Ni2+ low spin and Ni3+ symmetries does not change as particle size is reduced. X-ray magnetic circular dichroism studies show that the spin and orbital moments are parallel and that as particle size is decreased the orbital to spin moment ratio is increased from the bulk value of 17% to 25%. The development of the equipment and experimental technique of high pressure magnetic Compton scattering utilising a diamond anvil cell is discussed in detail. It is shown that this technique can be successfully applied to measure the one dimensional electron momentum densities of samples situated within the anvil cell. The development and adaptation of the cell for several complementary laboratory techniques is also discussed.
6

McNally, Graham Michael. "High pressure synthesis and neutron diffraction studies of new magnetic manganites". Thesis, University of Edinburgh, 2018. http://hdl.handle.net/1842/31185.

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With the discovery of appreciable room temperature magnetoresistance (MR) in high Curie temperature (Tc) ferrimagnetic double perovskites such as Sr2FeMoO6, research surrounding other materials of this type has expanded. Most ferrimagnetic double perovskites of the formula A2BB'O6 have non-magnetic A-site cations, such as Sr2+, Ca2+ or Ba2+. Replacing non-magnetic cations with magnetic variants offers further possibilities to tune magnetic effects. This thesis focuses on the substitution of non-magnetic A-site cations with relatively small magnetic Mn2+ cations. This substitution is made possible through the use of high-pressure/temperature (P/T) synthesis, and the characterisation of structural and magnetic properties of new phases discovered through these syntheses. The first of these new phases to be reported herein is Mn2FeReO6, which can be described as the Mn analogue of the well-known ferrimagnetic double perovskite Ca2FeReO6. These materials are well ordered with Fe3+/Re5+ on B-sites and crystallise in a P21/n structure. Mn2FeReO6 shows a high Tc of 520 K due to ferrimagnetic Fe/Re magnetic order above RT, and a large saturated magnetisation of 5.0 μB, which peaks at 75 K. Interestingly, the A-site Mn2+ (3d5) magnetic order has the effect of causing a spin reorientation of the Fe/Re sublattice observed by neutron powder diffraction (NPD) at temperatures below ~75 K. This causes the MR to exhibit the expected negative intergrain tunnelling behaviour above the transition and colossal positive behaviour below. Also reported are a series of perovskite related structures with formulae CaxMn2- xFeReO6 (x = 0.5, 1.0, 1.5). Of particular note among these is CaMnFeReO6, which exhibits 1:1 A-site ordering of Ca/Mn and adopts the P42/n space group. This material belongs to a family of newly discovered 'double double' perovskites, in which Ca/Mn order in columns pointing along the c-axis and Mn has alternating tetrahedral and square planar coordination environments. MR in this material remains negative down to 20 K, potentially due to the presence of Ca disrupting magnetic interactions between Mn2+ cations and suppressing the spin transition. Alternating coordination environments in the double double perovskite structure type were exploited in the synthesis of Ca(Mn0.5Cu0.5)FeReO6. This material also crystallises in the P42/n structure and is well ordered on B-sites, as evidenced by X-ray powder diffraction. Neutron diffraction yields, in addition to columnar order, a slight preference for Cu to occupy the square planar sites and for Mn to occupy tetrahedral sites. This doping of square planar sites with Cu has the effect of enhancing magnetic properties compared to CaMnFeReO6, increasing the saturated magnetisation, raising the ferrimagnetic ordering temperature of the B-sites from 500 to 560 K, and also having a profound effect on the observed MR effects, as a switch in the sign of the MR is observed in this material through a magnetic transition. Finally, B-site substitution has been experimented with in the synthesis of CaMnMnReO6. This also possesses the combined A and B-site orders observed in CaMnFeReO6 and an unusual magnetic structure, with perpendicular A and B-site magnetism due to frustration, deviating greatly from the magnetic structures of materials with B-site Fe/Re. In summary, this thesis compiles the synthesis and analysis of a series of new double perovskites, double double perovskites and a new 'triple double' five-fold cation ordered structure with a general formula of AA'0.5A''0.5BB'O6. These materials show that new types of structural ordering can be used to increase the number of degrees of freedom available for tuning the interplay between many different magnetic cations in different coordination environments.
7

Sokolov, Dmitriy A. "Effect of pressure on transport and magnetic properties of layered manganites". Thesis, University of Edinburgh, 2002. http://hdl.handle.net/1842/14442.

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8

Rochette, P., G. Fillion, R. Ballou, F. Brunet, B. Ouladdiaf e L. Hood. "High pressure magnetic transition in pyrrhotite and impact demagnetization on Mars". AMER GEOPHYSICAL UNION, 2003. http://hdl.handle.net/10150/623401.

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Using neutron diffraction under pressure at room temperature, we observed that pyrrhotite undergoes a ferrimagnetic to paramagnetic transition at about 2.8 GPa. Complete demagnetization of remanence at the same pressure is confirmed in an independent experiment. Such a process provides a quantitative explanation of the magnetic structure of the Martian Southern Hemisphere assuming that pyrrhotite is the major magnetic mineral and that our static experiments can be extrapolated to dynamic pressure conditions. Indeed, the 3 GPa isobaric line during the two large impacts of Argyre and Hellas separates the magnetized and unmagnetized zones. We also infer a reinterpretation of Martian meteorites paleomagnetic signal.
9

Prescimone, Alessandro. "Effect of high-pressure on molecular magnetism". Thesis, University of Edinburgh, 2010. http://hdl.handle.net/1842/4619.

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The effect of pressure on a number of magnetically interesting compounds such as single-molecule magnets and dimeric copper and manganese molecules has been investigated to probe the validity of ambient magneto-structural correlations. The first chapter is an introduction to the equipment and methodologies that have been adopted to carry out the experimental high-pressure work. The second chapter reports the first combined high-pressure single crystal X-ray diffraction and high pressure magnetism study of four single-molecule magnets (SMMs). At 1.5 GPa the structures [Mn6O2(Et-sao)6(O2CPh(Me)2)2(EtOH)6] (1) – an SMM with a record effective anisotropy barrier of ~86 K – and [Mn6O2(Etsao) 6(O2C-naphth)2(EtOH)4(H2O)2] (2) both undergo significant structural distortions of their metallic skeletons which has a direct effect upon the observed magnetic response. Up to 1.5 GPa pressure the effect is to flatten the Mn-N-O-Mn torsion angles weakening the magnetic exchange between the metal centres. In both compounds one pairwise interaction switches from ferro- to antiferromagnetic, with the Jahn-Teller (JT) axes compressing (on average) and re-aligning differently with respect to the plane of the three metal centres. High pressure dc χMT plots display a gradual decrease in the low temperature peak value and slope, simulations showing a decrease in |J| with increasing pressure with a second antiferromagnetic J value required to simulate the data. The “ground states” change from S = 12 to S = 11 for 1 and to S = 10 for 2. Magnetisation data for both 1 and 2 suggest a small decrease in |D|, while out-of-phase (χM //) ac data show a large decrease in the effective energy barrier for magnetisation reversal. The third SMM is the complex [Mn3(Hcht)2(bpy)4](ClO4)3·Et2O·2MeCN (3·Et2O·2MeCN) that at 0.16 GPa loses all associated solvent in the crystal lattice, becoming 3. At higher pressures structural distortions occur changing the distances between the metal centres and the bridging oxygen atoms making |J| between the manganese ions weaker. No significant variations are observed in the JT axis of the only MnIII present in the structure. Highpressure dc χMT plots display a gradual decrease in the low temperature peak value and slope. Simulations show a decrease in J with increasing pressure although the ground state is preserved. Magnetisation data do not show any change in |D|. The fourth SMM, [(tacn)6Fe8O2(OH)12](ClO4)3.9Br4.1⋅6H2O, (4) is the largest inorganic compound ever studied at high-pressure. Up to 2.0 GPa the conformation of the complex remains largely unaffected, with the counter ions and water molecules moving around to accommodate a compression of the unit cell volume. High pressure magnetic susceptibility data collected up to 0.93 GPa confirm minimal changes in the intra-molecular exchange interactions. The third chapter focuses on three hydroxo-bridged CuII dimers: [Cu2(OH)2(H2O)2(tmen)2](ClO4)2 (5), [Cu2(OH)2(tben)2](ClO4)2 (6) and [Cu2(OH)2(bpy)2](BF4)2 (7) have been structurally determined up to 2.5, 0.9 and 4.7 GPa, respectively. 6 and 7 have never been reported before. Pressure imposes important distortions in the structures of all three complexes, particularly on the bond distances and angles between the metal centres and the bridging hydroxo groups. 5 undergoes a phase transition between 1.2 and 2.5 GPa caused by the loss of a coordinated water molecule. This leads to a loss of symmetry and dramatic changes in the molecular structure of the complex. The structural changes are manifested in different magnetic behaviours of the complexes as seen in dc susceptibility measurements up to ~0.9 GPa: J becomes less antiferromagnetic in 5 and 6 and more ferromagnetic in 7. The fourth chapter shows the compression of two oxo-bridged MnII/MnIII mixed valence dimers: [Mn2O2(bpy)4](ClO4)3⋅3CH3CN, (8) has been squeezed up to 2.0 GPa whilst [Mn2O2(bpy)4](PF6)3⋅2CH3CN⋅1H2O, (9) could be measured crystallographically up to 4.55 GPa. 9 has never been reported before, while 8 has been reported in a different crystallographic space group. The application of pressure imposes significant alterations in the structures of both complexes. In particular, in 8 the Mn-Mn separation is reduced by the contraction of some of the Mn-O bond distances, 9 shows essentially analogous behaviour: the Mn-Mn distance and nearly all the Mn-N bonds shrink significantly. The magnetic behaviour of the complexes has been measured up to 0.87 GPa for 8 and 0.84 GPa for 9, but neither display any significant differences with respect to their ambient data.
10

Lenfeldt, Niklas. "The search for reversibility of idiopathic normal pressure hydrocephalus : aspects on intracranial pressure measurements and advanced MRI techniques in combination with CSF volume alteration /". Umeå : Univ, 2007. http://urn.kb.se/resolve?urn=urn:nbn:se:umu:diva-1422.

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Libri sul tema "Magnetic pressure":

1

Kawazoe, Yoshiyuki, Takeshi Kanomata e Ryunosuke Note. High Pressure Materials Properties: Magnetic Properties of Oxides Under Pressure. Berlin, Heidelberg: Springer Berlin Heidelberg, 2023. http://dx.doi.org/10.1007/978-3-662-64593-2.

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2

J, Jonas, e Akitt J. W, a cura di. High pressure NMR. Berlin: Springer-Verlag, 1991.

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3

1931-, Akitt J. W., e Jonas Jiri, a cura di. High pressure NMR. Berlin: Springer, 1991.

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4

D, Leighty Bradley, e Langley Research Center, a cura di. Portable digital pressure indicator for calibrating magnetic recorders. Hampton, Va: National Aeronautics and Space Administration, Langley Research Center, 1990.

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5

Kaneko, T., e T. Kanomata. Magnetic Properties of d-Elements, Alloys and Compounds Under Pressure. A cura di Y. Kawazoe, T. Kaneko e Y. Uwatoko. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41834-1.

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6

Sh, Boltachev G., a cura di. Magnetic pulsed compaction of nanosized powders. Hauppauge, N.Y: Nova Science, 2009.

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7

C, Begelman Mitchell, e United States. National Aeronautics and Space Administration., a cura di. Radiation pressure-driven magnetic disk winds in broad absorption line quasi-stellar objects. [Washington, DC: National Aeronautics and Space Administration, 1995.

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C, Begelman Mitchell, e United States. National Aeronautics and Space Administration., a cura di. Radiation pressure-driven magnetic disk winds in broad absorption line quasi-stellar objects. [Washington, DC: National Aeronautics and Space Administration, 1995.

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9

United States. National Aeronautics and Space Administration., a cura di. Study of some superconducting and magnetic materials on high Tc oxide superconductors: Final report, grant no. NAG8-032, June 1985 - September 1987. [Washington, DC: National Aeronautics and Space Administration, 1987.

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10

1882-1973, Spence H. E., Stern D. P e United States. National Aeronautics and Space Administration., a cura di. Empirical modeling of the quiet time nightside magnetosphere. [Washington, D.C: National Aeronautics and Space Administration, 1993.

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Capitoli di libri sul tema "Magnetic pressure":

1

Baudelet, François. "High-Pressure Magnetism and Magnetic Circular Dichroism". In Magnetism and Synchrotron Radiation, 254–72. Berlin, Heidelberg: Springer Berlin Heidelberg, 2001. http://dx.doi.org/10.1007/3-540-44954-x_11.

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2

Hemley, Russell J., Ho-kwang Mao e Ronald E. Cohen. "Chapter 18. HIGH-PRESSURE ELECTRONIC AND MAGNETIC PROPERTIES". In Ultrahigh Pressure Mineralogy, a cura di Russell J. Hemley, 591–638. Berlin, Boston: De Gruyter, 1998. http://dx.doi.org/10.1515/9781501509179-020.

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3

Kobayashi, H., H. Ide, M. Kabuto, Y. Handa, H. Kawano e M. Hayashi. "Intracranial Pressure and Phosphorus-31 Magnetic Resonance Spectroscopy in Cats". In Intracranial Pressure VIII, 262–64. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-77789-9_55.

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4

Goncharenko, I. N. "Magnetic Properties of Crystals and their Studies at High-Pressure Conditions". In High-Pressure Crystallography, 321–40. Dordrecht: Springer Netherlands, 2004. http://dx.doi.org/10.1007/978-1-4020-2102-2_20.

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Raftopoulos, C., C. Chaskis, L. Bidaut, F. Cantraine, D. Balériaux, C. Matos, F. Delecluse e J. Brotchi. "Brain Edema Induced by Ventricular Puncture. A Study by Magnetic Resonance Imaging". In Intracranial Pressure VIII, 797–801. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-77789-9_175.

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Kawai, N., S. Nagao, M. Fujisawa, K. Fujita, T. Ito e T. Ohmoto. "Analysis of Pyramidal Tract Function in Experimental Intracranial Hypertension by Magnetic Stimulation". In Intracranial Pressure VIII, 214–20. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-77789-9_47.

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Yoshida, K., A. Marmarou e M. Furuse. "The Metabolic Protection of Hypoxia by Etomidate Evaluated by Magnetic Resonance Spectroscopy". In Intracranial Pressure VIII, 273–75. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-77789-9_58.

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Inao, S., H. Kuchiwaki, H. Kanaiwa, K. Sugita, S. Takada, A. Izawa e M. Furuse. "Assessment of Brainstem Distortion Associated with Extraaxial Supratentorial Mass by Magnetic Resonance Imaging". In Intracranial Pressure VIII, 79–81. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-77789-9_17.

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9

Pasternak, M. P., G. Kh Rozenberg, W. M. Xu e R. D. Taylor. "Electronic, Structural, and Magnetic Properties of Transition-Metal Insulators at Very High Pressures". In High-Pressure Crystallography, 311–20. Dordrecht: Springer Netherlands, 2004. http://dx.doi.org/10.1007/978-1-4020-2102-2_19.

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Kawazoe, Yoshiyuki, Takeshi Kanomata e Ryunosuke Note. "ScCrO3 (Synthesized Under Pressure)". In High Pressure Materials Properties: Magnetic Properties of Oxides Under Pressure, 234–37. Berlin, Heidelberg: Springer Berlin Heidelberg, 2023. http://dx.doi.org/10.1007/978-3-662-64593-2_54.

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Atti di convegni sul tema "Magnetic pressure":

1

Song, Pan, Xiaoying Tang, ShaoJun Wang, Bin Ren, Yantian Zuo e Jielu Wang. "A Study on the Magnetic Distribution of Nd-Fe-B Permanent Magnets in Pipeline in Line Inspection Tool". In ASME 2018 Pressure Vessels and Piping Conference. American Society of Mechanical Engineers, 2018. http://dx.doi.org/10.1115/pvp2018-84529.

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Abstract (sommario):
The pressure pipeline in line inspection technology is the most effective nondestructive testing method to detect the quality of buried oil and gas pipelines at present. In line inspection tool usually uses magnetic flux leakage (MFL) technology to detect the change of leakage magnetic field to detect pipeline defects. Permanent magnets magnetize the wall of the pipeline as an excitation. During the detection process, the magnetic field performance of permanent magnets is required to be high. At the same time, the magnetic performance of the permanent magnet in the magnetic cleaning pipe also determine the cleaning effect inside the pipeline. In this paper, the magnetic distribution of permanent magnets is studied and the Nd-Fe-B permanent magnets with the best magnetic properties are taken as the objects. The finite element simulation is used to optimize the shape of the permanent magnets with better magnetic distribution, and the magnetic intensity factors of the preferred cylindrical permanent magnets are analyzed. In addition, three experiments of the influence of temperature, the influence of the ferromagnetic combination, and the influence of the environment medium are conducted. As a result, the relationship between the magnetic intensity of the Nd-Fe-B permanent magnets and the factors is obtained. The conclusion is of great significance to the design and research of permanent magnetic circuit in line inspection magnetization device.
2

Zhang, Hongsheng, Yanbin Li, Kai Guo e Jianxv Jiang. "An Active Magnetic Saddle Based on Electro-Permanent Magnetic Adhesion Mechanism". In ASME 2022 Pressure Vessels & Piping Conference. American Society of Mechanical Engineers, 2022. http://dx.doi.org/10.1115/pvp2022-84528.

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Abstract In this paper, a novel transport technique for pressure vessels based on electro-permanent magnet (EPM) technology is proposed. The magnetic force and the resulting transport gripping force (TGF) are applied by controllable permanent magnets rather than conventional electromagnet or permanent magnet technology, and the current is only required at the moment of loading or unloading the TGF. The EPM system is convenient in control, and low in energy consumption. The experimental device including magnetic chuck, web of foundation girder and other components is constructed based on the EPM characteristics and requirements of transported equipment. The EPM units are used to generate magnetic force to realize loading and unloading of TGF. The principles and advantages of EPM transport technique are first elaborated with theoretical derivation and magnetic field simulation. Then, a series of experiments such as electrical circuit, magnetic field and tensile test were performed for the EPM chuck and magnetic saddle. It is demonstrated that the TGF applied by the designed system is large enough for the transportation of the pressure vessel. Also, the energy saving is significant using the EPM transportation system.
3

Nakasone, Yuji, e Yoshifumi Iwasaki. "FEM Analysis of Magnetic Field Induced by Martensitic Phase Transformation Around Fatigue Cracks in SUS 304 Stainless Steel". In ASME/JSME 2004 Pressure Vessels and Piping Conference. ASMEDC, 2004. http://dx.doi.org/10.1115/pvp2004-2769.

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Abstract (sommario):
The present study has attempted to analyze the distributions of vertical magnetic flux density Bz above growing fatigue cracks subjected to various stress ratios R in SUS 304 stainless steel in which plasticity-induced martensitic transformation has occurred at room temperature in air. FEM calculations have been made to obtain Bz distributions above fatigue cracks by using composite permanent magnet models. The martensitic transformation regions around fatigue cracks were modeled as composites of permanent magnets having different B-H properties varying according to the content of α′ martensitic phase transformed. The resultant distributions of leakage magnetic flux density above fatigue cracks obtained by FEM agree well with those obtained by experiments.
4

Sunakoda, Katsuaki, Shin Morishita, Seiichi Takahashi e Toshiyuki Hakata. "Development and Testing of Hybrid Magnetic Responsive Fluid for Vibration Damper". In ASME 2009 Pressure Vessels and Piping Conference. ASMEDC, 2009. http://dx.doi.org/10.1115/pvp2009-77651.

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A new intelligent fluid is studied and developed. Rheological characteristics of the developed fluid change rapidly and can be controlled in the presence of an applied magnetic field. The developed fluid is a hybrid type fluid, and it consists consisting of carbonyl irons and super fine magnetite. Average diameters of carbonyl iron and super fine magnetite are a size in the order of a few microns and about 10 nano-meters respectively. Special treatment is made by coating the surface of carbonyl iron with super fine magnetite. Physical properties such as dispersion stability and thixotropical characteristics are examined. Shearing stress and pressure drops of the new fluid flow are examined and evaluated by changing the strength of magnetic fields. A small capacity damper is made, and damping tests are performed using the new fluids and also commercial MR fluid. Dynamic properties of the damper are evaluated. As a result of a series of studies, the developed hybrid magnetic responsive fluid is expected to be used as an intelligent fluid.
5

Matsuoka, Taichi, e Katsuaki Sunakoda. "Application of Electromagnet Using Magnetization or Demagnetization for Magnetic Damper". In ASME 2008 Pressure Vessels and Piping Conference. ASMEDC, 2008. http://dx.doi.org/10.1115/pvp2008-61141.

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In this paper the authors develop a new type of a hybrid magnetic damper which has a variable damping force generated by hybrid electromagnets. The hybrid electromagnet is composed of a ferrite core combined with a rare-earth magnet. The damper can make the damping coefficient increasing from neutral value with magnetized field, or otherwise decreasing it with demagnetized field. It has also a fail-safe mechanism under an electrically malfunction. In order to determine the magnetic damping coefficients created by eddy current depend on a shape of a magnet and a conductive disk, it is accurately calculated by using an arc shape. For investigating about dynamic properties, resisting force characteristics are measured by using a vibration actuator. In experimental results, the damper has a damping coefficient which is proportional to current squared increasing and decreasing from neutral value. Seismic response simulations of one-degree-of-freedom system with the hybrid damper are calculated using LQR control. The effects of vibration suppression are confirmed numerically.
6

Krejci, Petr, e Cestmir Ondrusek. "Design Optimization of Magnetic Coupling Using Genetic Algorithm and 2D FEM Model". In ASME/JSME 2004 Pressure Vessels and Piping Conference. ASMEDC, 2004. http://dx.doi.org/10.1115/pvp2004-2313.

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Abstract (sommario):
Magnetic couplings (Figure 1) are widely used to torque transmission between two shafts without any mechanical contact. They are especially well suited for used in hazardous environments, to transmit torque through a separation wall. An additional advantage of a magnetic coupling is that slipping occurs when excessive torque is applied, this can be used to prevent mechanical failure due to torque overloads. This paper deals with influence of temperature on behavior of magnetic coupling and magnetic coupling design optimization. The permanent magnets that are used for torque transmission cannot be used close to Currie point, which is a point of loss of magnetic characteristics. We intend to use the magnetic coupling for pump of radioactive liquid materials for transmutation devices, where the temperature is close to four hundred centigrade. Because of we suggest the design changes for elimination of temperature influence. This paper presents the finite element (FE) parametric model of magnetic coupling, experimental verification of FE model and optimization of the inner part of magnetic coupling in order to increase the maximal torque. The genetic algorithm method in connection with FEM model of magnetic coupling was used for the design optimization procedure.
7

Wei, Haotian, Shaohua Dong, Yundong Ma, Lushuai Xu, Jiahao Zhao e Hang Zhang. "Simulation Analysis and Experimental Study on Pipeline Circumferential Crack Detection Based on Residual Magnetism Effect". In ASME 2023 Pressure Vessels & Piping Conference. American Society of Mechanical Engineers, 2023. http://dx.doi.org/10.1115/pvp2023-105782.

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Abstract A method for crack detection on the surface of pipelines that uses residual magnetic detection technology based on the hysteresis effect after magnetizing the pipeline to magnetic saturation has been developed in this study. Support vector regression (SVR) was employed for quantitative assessment. This paper reviewed the magnetization process of the magnetizer, the generation of residual magnetism effect, and the detection of residual magnetic fields. An experimental and theoretical study examined how the crack size affects residual magnetic anomalies. The simulation results indicated that the characteristic values of the residual magnetic anomaly changed in a roughly linear fashion at a more significant crack depth. As the crack width increased, the variations in residual magnetic anomaly characteristic quantities were relatively mild. The input values were denoted by the extracted characteristic amounts. The width and depth parameters of the crack were used as output values. A trained SVR model was employed to estimate the crack size. The crack widths and depths were accurately determined at 62.5% and 85.42%, respectively by combining this detection method, SVR, and the experimental results. This study demonstrated the feasibility of using residual magnetic detection technology, combined with SVR, to detect circumferential cracks in pipelines, which is an essential supplement to internal magnetic flux leakage detection and assessing pipelines.
8

Lee, Taeseung, Jong Hyuk Lee e Yong Hoon Jeong. "Pool Boiling and Flow Boiling CHF Enhancement at Atmospheric Pressure Using Magnetic Nanofluid". In 2012 20th International Conference on Nuclear Engineering and the ASME 2012 Power Conference. American Society of Mechanical Engineers, 2012. http://dx.doi.org/10.1115/icone20-power2012-55094.

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In this study, we suggest a new working fluid: magnetic nanofluid, or magnetite-water nanofluid, which is a colloidal suspension of magnetite nanoparticles in the pure water. By using the nanofluid, we can expect the critical heat flux (CHF) enhancement, and also for the magnetic nanofluid. Since the magnetite nanoparticles can be controlled by an external magnetic field, the magnetic nanofluid is regarded as a controllable nanofluid, and thus, we can expect the advantages of magnetic nanofluid: 1) the nanoparticle suspension in nanofluid can be maintained by applying the alternating magnetic field, 2) the nanofluid concentration can be localized by applying the magnetic field for a region of interest and 3) the magnetite nanoparticles can be removed from magnetic nanofluid easily. In this study, we focused on the CHF characteristics of magnetic nanofluid in both pool boiling and flow boiling. The first part is for the pool boiling CHF of magnetic nanofluid. At atmospheric pressure, saturated pool boiling CHF experiments were conducted using Ni-Cr wire for magnetic nanofluid and the other nanofluids. Among the various nanofluids, magnetic nanofluid has the highest value of pool boiling CHF, and the enhancement ratio (with respect to the pure water) ranges from 170 to 240 percent. To elucidate the mechanism underlying the pool boiling CHF enhancement, three approaches were introduced: 1) scanning electron microscope (SEM) images were obtained to explain the pool boiling CHF enhancement mechanism due to the deposited nanoparticles, which is related to the surface wettability of the heat transfer surface, 2) ultra-high speed movie were taken and analyzed to observe the bubble dynamics at the heat transfer surface and 3) the strength of electricity-induced magnetic field neat the heat transfer surface were calculated to examine the effect of magnetic field on the pool boiling CHF. The second part is for the flow boiling CHF of magnetic nanofluid. A series of flow boiling CHF experiments were performed at atmospheric pressure and low mass flux conditions. Based on the experimental data, we conclude that the use of magnetic nanofluid improves the flow boiling CHF characteristics: the flow boiling CHF enhanced for the magnetic nanofluid. This is mainly due to the deposition of magnetite nanoparticles on the heat transfer surface, which results in the improvement of wettability and re-wetting characteristics. And we need enough time to ensure the nanoparticle deposition and the flow boiling CHF enhancement, when a nanofluid is used as a working fluid.
9

Sodeyama, Hiroshi, Kazuhiko Shibata, Yusuke Sato, Tetsuya Tomizawa e Hideo Fujitani. "A Study on Controllable Aseismic Device With Inertia Mass and MR Fluid". In ASME 2013 Pressure Vessels and Piping Conference. American Society of Mechanical Engineers, 2013. http://dx.doi.org/10.1115/pvp2013-97650.

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The authors have developed a new aseismic device, which has a ball screw and rotational mass. It not only generates the resistive inertial force originating in the rotational mass but also dissipates the energy of vibration through a viscous damping mechanism. Furthermore, the damping capability of the device can be controlled externally with an applied magnetic field. A magneto-rheological (MR) fluid is used to change the dynamic characteristics of the device. Through comprehensive experimental testing of a prototype device, the dynamic characteristics of the device have been verified. The test results show that the force-displacement relationship varies with an applied magnetic condition. Only a few amperes of electric current is required to generate a magnetic field effective for the prototype device with a capacity of 100kN.
10

Mo^ri, Nobuo. "Electrical and magnetic properties of Ce monopnictides". In High-pressure science and technology—1993. AIP, 1994. http://dx.doi.org/10.1063/1.46260.

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Rapporti di organizzazioni sul tema "Magnetic pressure":

1

S.R. Hudson & N. Nakajima. Pressure, Chaotic Magnetic Fields and MHD Equilibria. Office of Scientific and Technical Information (OSTI), maggio 2010. http://dx.doi.org/10.2172/981705.

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2

H.E. Mynick and A.H. Boozer. Anisotropic Pressure, Transport, and Shielding of Magnetic Perturbations. Office of Scientific and Technical Information (OSTI), maggio 2008. http://dx.doi.org/10.2172/960291.

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Neef, W. S. Beryllium pressure vessels for creep tests in magnetic fusion energy. Office of Scientific and Technical Information (OSTI), luglio 1990. http://dx.doi.org/10.2172/6681479.

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4

Gangrao, Hota V. S., Udaya B. Halabe, John Zondlo, Mark Skidmore, Ben Imes, Jonas Kavi, Andrew Pacifico, Ronald Alexander, Andrew Cvetnick e Patrick Sisler. DTPH56-16-HCAP-02 Glass-Polymer Composite High Pressure Pipes and Joints-Design, Manufacture. Chantilly, Virginia: Pipeline Research Council International, Inc. (PRCI), settembre 2018. http://dx.doi.org/10.55274/r0011841.

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The project focuses on developing glass fiber reinforced polymer (GFRP) composite pipes including a range of joining systems. A few of the many advantages of GFRP composite pipes are their non-corrosiveness, magnetic transparency, and high strength-to-weight ratio. As a part of this project, GFRP pipes and joints were designed, manufactured, and evaluated under static loads. Emphasis was placed in the evaluation of stress-rupture (burst pressure) of GFRP composite pipes that could withstand internal pressures as high as 5000 psi. The report also includes the design and testing of high-pressure composite joints for these pipes. In addition, the report discusses the use of Ground Penetrating Radar (GPR) for successfully detecting the FRP pipes under buried conditions. The report also includes the detection of gas leakage from buried pipes using mass spectroscopy.
5

Hegna, C. C., e J. D. Callen. Pressure profiles, resonant Pfirsch-Schlueter currents, thermal instabilities and magnetic island formation. Office of Scientific and Technical Information (OSTI), giugno 1992. http://dx.doi.org/10.2172/10150519.

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6

Hegna, C. C., e J. D. Callen. Pressure profiles, resonant Pfirsch-Schlueter currents, thermal instabilities and magnetic island formation. Office of Scientific and Technical Information (OSTI), giugno 1992. http://dx.doi.org/10.2172/5166537.

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7

NASH, THOMAS J. Adiabatic Quasi-Spherical Compressions Driven by Magnetic Pressure for Inertial Confinement Fusion. Office of Scientific and Technical Information (OSTI), novembre 2000. http://dx.doi.org/10.2172/771501.

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8

Xie, Weiwei. Unraveling Emergent Quantum States in Magnetic Topological Insulators using High Pressure Neutron Scattering. Office of Scientific and Technical Information (OSTI), luglio 2023. http://dx.doi.org/10.2172/2326931.

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9

Bykov, A. I., G. V. Boriskov e M. I. Dolotenko. Condensed argon isentropic compression with ultrahigh magnetic field pressure: Experimental design. Post-shot report. Office of Scientific and Technical Information (OSTI), dicembre 1996. http://dx.doi.org/10.2172/564275.

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10

Tokuo, Kenichiro, Kenji Hiraku e Hiroyuki Yamada. Integration of Magnetic Solenoid Valve Model Into High-Pressure Fuel Pump Simulator and Its Application. Warrendale, PA: SAE International, maggio 2005. http://dx.doi.org/10.4271/2005-08-0013.

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