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Toshiyuki Ishimatsu, Takemi Nakagawa, Hikonojo Orihara, Haruko Ohmura, ...
1971 Volume 30 Issue 6 Pages
1519-1522
Published: June 15, 1971
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The
116Cd(
3He, d)
117In reaction has been studied with a 25.07 MeV
3He beam. The
l values and spectroscopic strengths were determined for ten levels up to 2.0 MeV excitation. Strong
l=0 and 2 transitions were observed against the simple shell-model expectation. These transitions are compared with predictions of the rotational model proposed by several authors, and significant disagreements are found.
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Katsumichi Suzuki, Noriaki Takahashi, Takahisa Itahashi, Tetsuo Wakats ...
1971 Volume 30 Issue 6 Pages
1523-1534
Published: June 15, 1971
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The nuclear structures of
38K and
38Cl are investigated by
40Ca(
d, α)
38K and
40Ar(
d, α)
38Cl reactions with 11.4 MeV deuterons. The excitation functions for
40Ca(
d, α)
38K reaction have been obtained for the deuteron energy between 10.65 and 12.17 MeV. The angular distributions have been measured on the low excited states of
38K and
38Cl. The zero range DWBA analysis of the angular distributions on these excited states gives the spin, parity and isospin assignments as follows, the 2.63 MeV state (4, 3 or 2)
−0, the 2.85 MeV state (4, 3 or 2)
−0 and the 3.97 MeV state (3, 2 or 1)
+0 for
38K. Four strongly excited states are found in
38Cl at 1.82, 1.99, 2.51 and 2.82 MeV and are considered to have positive parity from DWBA calculations. The spin and parity are considered tentatively to be (3)
+ for the 1.99 MeV state in
38Cl.
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Takeshi Saito
1971 Volume 30 Issue 6 Pages
1535-1545
Published: June 15, 1971
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A total of 7695 heavy nuclei were located in the Brawley emulsion stack. The error in energy estimation was about 30% and that in charge estimation was 0.25 units of charge for nuclei with
z≤9 and 0.5 for the iron group. The flux values for respective charge groups at the top of the atmosphere at energies above 10 GeV/nucleon are
JM0=0.686±0.117,
JH0=0.241±0.032,
JLH0=0.166±0.022,
JMH0=0.015±0.004 and
JVH0=0.060±0.012, particles/m
2·sec·sterad. The integral energy spectra of the individual charge groups have the same exponent of γ=1.60 up to several hundreds of GeV/nucleon. On the basis of the experimental results in the present investigation, the mechanisms of cosmic ray acceleration and the amount of matter traversed by the cosmic rays are discussed.
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Shin-ichi T. Inoue, Setsuro Asano, Jiro Yamashita
1971 Volume 30 Issue 6 Pages
1546-1554
Published: June 15, 1971
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Fermi surfaces of all alkali metals are evaluated by A.P.W. method with various crystal potentials, which include the Wigner-Seitz potential, Hartree-Fock-Slater self-consistent crystal potential and the Heine-Hedin type potential. The results are compared with available experiments. The purpose of the calculation is to examine the accuracy of the
ab initio calculation to reproduce the observed Fermi surface, and also to examine what potential is the best.
It is found that the original Wigner-Seitz potential is a fairly good potential, but not the best one. It is suggested that the best potential should include the effects of the crystal.
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Kikuo Cho, Yutaka Toyozawa
1971 Volume 30 Issue 6 Pages
1555-1574
Published: June 15, 1971
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Optical properties of interacting exciton-phonon system have been theoretically studied in terms of a simple model consisting of Frenkel excitons and Einstein oscillators. The problem is characterized by two non-dimensional parameters
B and
S representing the exciton band width and the interaction energy, respectively. Approximate solutions have been obtained through the diagonalization of the Hamiltonian in special sub-spaces, and they reasonably describe the behavior of the system for all values of
B and
S. Absorption and emission spectra and the effective mass of the composite particle vary from free exciton type to self-trapped exciton type as we go from
B>
S to
B<
S. The energy-momentum relation has been qualitatively studied below the one-phonon continuum, and the following new features have been found in the strong coupling region; (1) complete split-off of the lowest branch in the whole Brillouin zone, and (2) the split-off of the second discrete branch. Furthermore, a clue to the mechanism of the Urbach-Martienssen rule has also been obtained.
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Masahiro Inoue, Makoto Okazaki
1971 Volume 30 Issue 6 Pages
1575-1586
Published: June 15, 1971
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A relativistic formulation of the Korringa-Kohn-Rostoker method for band calculation is presented for non-muffin-tin potential. The method developed here includes the full relativistic effects together with the effect of the non-muffin-tin character which comes from the overlapping ionic potentials. The method is appropriate for the crystals of heavy elements, especially in a loosely packed structure.
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Takashi Iwashita, Toshihiro Idogaki, Norikiyo Uryû
1971 Volume 30 Issue 6 Pages
1587-1588
Published: June 15, 1971
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The exchange interactions in the quadri-nuclear complex compound in which the magnetic ions form a cluster of rhomboid structure are studied. In addition to the ordinary exchange interactions, the higher order spin coupling is shown to be necessary to interpret the magnetic susceptibility data.
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Eisuke Hayashi, Masao Shimizu
1971 Volume 30 Issue 6 Pages
1589-1595
Published: June 15, 1971
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The spin density induced by an impurity of transition elements in iron is investigated by taking into account the dielectric screening of an impurity charge and the local exchange enhancement. The Fourier transform of the induced spin density, the induced magnetic moment within an impurity cell and the change of the magnetization per impurity atom are calculated self-consistently. All the calculated results of these quantities for several kinds of impurities are consistent with the experimental results except the cases where the difference between valences of an impurity atom and an iron atom is less than −2. The observed characteristic difference between the distributions of magnetic moment induced by impurities of the left-hand and right-hand sides of iron in the periodic table is explained.
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Yoshihiko Nakagawa
1971 Volume 30 Issue 6 Pages
1596-1602
Published: June 15, 1971
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The magnetic domain wall images in permalloy and 5% Mo-permalloy with high magnetic permeabilities were observed by means of Lorentz microscopy. The specimens were of the form of thin films prepared by electrolysis of bulk materials.
Correlating these observations with the initial permeabilities, it was found that, as the initial permeabilities become high, the magnetic domain walls change their appearances from straight lines to curved lines and finally they vanish in part. In a local part about 20μ in diameter of the specimen with permeability at 0.001 Oe, μ
0.001=120,000, typical circularly magnetized domain pattern has been observed for the first time in a monograin state.
The energy calculation for this configulation with circular magnetization was performed. Comparing this result with that for a uniformly magnetized domain, the existence of the circularly closed magnetic domain in low effective anisotropy—high permeability—magnetic materials is justified.
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Izuru Kimura
1971 Volume 30 Issue 6 Pages
1603-1604
Published: June 15, 1971
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The values of the exchange constants in CoCl
2·6H
2O are estimated using the values of
TN,
TAE and χ
i(
T) obtained experimentally. The results are
J1=0.61
kB,
J2=0.46
kB and
J3=0.04
kB.
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Shoichi Tomiyoshi, Hisao Yamamoto, Hiroshi Watanabe
1971 Volume 30 Issue 6 Pages
1605-1613
Published: June 15, 1971
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Distribution of the internal magnetic fields and its temperature dependence of Fe
57 nuclei in fcc iron-nickel alloys with composition ranging from 31.8 to 65.6 at.% Ni have been measured by Mössbauer effect from 88°K to above Curie temperature. Distribution of the internal field has been determined from the observed Mössbauer spectra and temperature variation of the distribution has been explained by using the molecular field model which shows that iron moments on which weaker exchange field is acting from the neighbouring moments decrease more rapidly with increasing temperature than those on which stronger exchange field is acting. Distribution of the internal magnetic field has been correlated to the distribution of the exchange field. Temperature dependence of saturation magnetization and other magnetic properties of iron-nickel alloys has been discussed on the basis of local fluctuation of the exchange field.
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Yasuo Endoh, Yoshikazu Ishikawa
1971 Volume 30 Issue 6 Pages
1614-1627
Published: June 15, 1971
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The magnetic phase diagram of γ Fe–Mn alloys has been investigated in the whole range of composition by neutron diffraction and other techniques. The f.c.c. phase of Fe–Mn alloys with less than 40 at. % iron and more than 85 at. % iron was stabilized by addition of small amounts of copper and carbon respectively in the alloys. An antiferromagnetic long range order was detected in the whole range composition. The antiferromagnetism of this alloy system Fe
x–Mn
1−x was found to be classified into three distinct groups according to the composition. They are 1) 0≤
x≤0.3, 2) 0.4<
x<0.8, and 3) 0.8≤
x≤1. The magnetic phase of the second group is markedly different from other two groups. The results agree qualitatively with the prediction based on the band theory.
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Hiroyuki Harada, Shin-ichiro Narita
1971 Volume 30 Issue 6 Pages
1628-1639
Published: June 15, 1971
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Reststrahlen reflectivities and localized vibration modes due to light impurities have been measured on Zn
xCd
1−xTe alloys.
Each reflection spectrum of these alloys exhibits clear “two-mode” behavior and shows no complex fine structure. Therefore, the theoretical analysis of the spectra can be done relatively easily and simply by developing a modified random-element-isodisplacement model.
The localized vibrations of impurities (S, Mg, Be) in Zn
xCd
1−xTe are explained by a model of the charged particles in a static parabolic potential well being affected by the local conditions in the alloy lattice.
The constants assumed in the analysis of the reflectivity spectra are consistent with the data in the localized vibrations.
Considering these results, a criterion has been proposed to determine whether a certain mixed crystal will exhibit “one-mode” or “two-mode” behavior.
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Mitsuhiro Takata, Soichi Oshida
1971 Volume 30 Issue 6 Pages
1640-1644
Published: June 15, 1971
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The pressure dependence of the thermodynamic critical field of La has been measured, and calculated the pressure effect on the electronic density of states at the Fermi surface is calculated.
The value of d ln
N(0)⁄d ln
v is found to be −4.54±1.67, where
N(0) and
v are the density of states at the Fermi surface and the volume respectively.
From the pressure dependence of
N(0) and
Tc of La-1.0%Ce, d ln
J⁄d ln
v is calculated to be −4.3 (
J is the exchange interaction parameter). From the experimental result, the mechanism of superconductivity of La at high pressure is discussed.
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Susumu Kurita, Koichi Kobayashi
1971 Volume 30 Issue 6 Pages
1645-1653
Published: June 15, 1971
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Oscillatory magneto-absorptions due to excitons have been studied in TlCl and TlBr. In zero magnetic field, absorptions due to exciton-phonon quasibound state and one and two free-phonon states of exciton quasicontinuum are observed. In magnetic field, members of
s exciton series with a subsidiary peak on the high energy side appear. The exciton binding energy is 11.7 meV in TlCl and 9.8 meV in TlBr and the reduced mass is 0.24
4m0 in TlCl and 0.23
4m0 in TlBr. A direct evidence of exciton polaron effect is obtained by observing the clamping of zero-phonon exciton lines of high quantum number in the vicinity of one free-phonon threshold of 2
s exciton. Above the threshold, absorptions of another series grow as the field increases. They are one-phonon replicas of zero-phonon excitons in magnetic field. The existence of two minima in the conduction band of each halide is suggested.
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Tsuneaki Goto, Katsuyuki Nishimura, Shigeharu Kabashima, Tatsuyuki Kaw ...
1971 Volume 30 Issue 6 Pages
1654-1661
Published: June 15, 1971
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In order to investigate the spin relaxation mechanism in Ti-doped VO
2 in relation to the itineracy of electrons associated with Ti impurities substituted for V
4+, the linewidth and line intensity of ESR absorption at 24 GHz have been measured on samples doped with various concentrations of Ti in a temperature range between 4.2 and 250 K. The spectrum with
hfs lines is observed at low concentration of Ti, while a single narrowed line of absorption is found at higher concentration. The temperature dependence of linewidth and line intensity of this single absorption line are discussed with respect to the staying time of electrons in the impurity state and their motions between impurity centers. The hopping frequency of electrons and the staying time in the impurity state are determined.
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Hiroshi Kukimoto, Shigeo Shionoya, Taibun Kamejima
1971 Volume 30 Issue 6 Pages
1662-1668
Published: June 15, 1971
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As to such Cd(S, Se) crystals that the position of the intrinsic A exciton coincides with the 488.0 nm argon ion laser line, photoconductivity and emission spectra were measured at 1.8°K under this laser line excitation. Photo-current increases in proportion to the square of excitation intensity above a certain critical excitation level. This gives direct evidence for free carrier generation from high density exciton state due to exciton-exciton interaction. At higher excitation levels a new emission line due to exciton-exciton interaction appears at a position shifted by the amount of the ionization energy of the intrinsic exciton from either the intrinsic or bound exciton line, providing further evidence. The emission peaks of the intrinsic and bound excitons shift to the opposite directions with increasing excitation intensity. This is interpreted as the consequence of the screening effect mutually exerted between the two kinds of excitons.
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Takeshi Miyanaga, Ken-ichi Kan’no, Shun-ichi Naoé, Hiroak ...
1971 Volume 30 Issue 6 Pages
1669-1675
Published: June 15, 1971
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The EPR spectra of a Ag
++ ion in CdCl
2 are studied at liquid nitrogen temperature and at room temperature. The Ag
++ ion is found at the center of the octahedron of six Cl
− ions. The octahedron of Cl
− ions is elongated tetragonally due to a Jahn-Teller effect at liquid nitrogen temperature. It is also observed that the principal axis of the
g-tensor deviates from a line joining the Ag
++ ion and one of the nearest neighbor Cl
− ions towards the crystal
c-axis. This deviation is interpreted to be due to the influence of the axial symmetry field parallel to the
c-axis on the Jahn-Teller effect. At room temperature a single broad EPR line with axial symmetry is observed.
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Yasuhiko Fujii, Yasusada Yamada
1971 Volume 30 Issue 6 Pages
1676-1685
Published: June 15, 1971
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The x-ray critical scattering due to the polarization fluctuation in Tri-Glycine Sulphate in the vicinity of the ferroelectric Curie point (
TC=48°C) has been observed in order to clarify the nature of inter-dipolar interaction to cause its phase transition. The observed critical scattering intensity shows a strong anisotropy around the reciprocal lattice points, with very narrow width in the direction of the polar axis. Based on the Ising model, the result was analyzed and it was found that the observed anisotropy was due to the long range electrostatic interaction between constituent microscopic dipoles.
The critical behavior of the inverse correlation range, expressed as κ=
A(
T⁄
TC−1)
ν, is investigated. From the temperature dependence of the critical scattering, the following values are obtained in the
a-direction:
A=0.18
6Å
−1, ν=0.50
2. The value of the critical exponent ν is in good agreement with that obtained in the molecular field approximation.
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Youichi Akasaka, Kohzoh Masuda, Susumu Namba
1971 Volume 30 Issue 6 Pages
1686-1689
Published: June 15, 1971
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Radiation induced defects in naphthalene and anthracene single crystals irradiated with reactor neutron at 10°∼17°K were studied by ESR at 4.2°K, 77°K, and room temperature.
Initial radicals produced in naphthalene at low temperature have been identified to be α-naphthyl radical and isolated hydrogen atoms, whereas in anthracene 9-anthryl radical and isolated hydrogen atoms have been detected. At room temperature the ESR signals of these radicals disappear, and α-hydronaphthyl radicals and dibenzo-cyclohexadienyl radicals have been detected innaphthalene and anthrance, respectively. The results indicate the following processes in the radiation damage in naphthalene and anthracene: RH+Reactor Neutron→R
·+H
·, RH+H
·→RH
·2.
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Kouichi Okamoto, Takeo Ichinokawa, Yoshi-Hiko Ohtsuki
1971 Volume 30 Issue 6 Pages
1690-1701
Published: June 15, 1971
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Numerical calculations are performed for contribution of various kinds of inelastic scattering, valence electron excitations (including the plasmon excitation), core electron excitations and phonon excitations on Kikuchi pattern of Si single crystal. An explanation of defect Kikuchi band is proposed by considering inelastic scatterings in detail. Two negative circle regions on the Kikuchi band are found theoretically. Experimental results corresponding to these calculations are also presented.
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Isao Shimamura
1971 Volume 30 Issue 6 Pages
1702-1708
Published: June 15, 1971
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The Harris method of obtaining scattering phase shifts is applied to the s-wave elastic electron and positron scattering by hydrogen atoms by use of Schwartz-type correlated trial functions with 50 and 56 terms, respectively. Kohn-method calculations with the same trial functions are also carried out at the same energies. The agreement between the Harris-method results and the Kohn-method results is good especially at low energies. In the electron-scattering case, two kinds of errors cancel each other to some extent, but in the positron case, they add up to make the agreement between the Harris-method and Kohn-method results somewhat worse.
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Kazunari Ikuta
1971 Volume 30 Issue 6 Pages
1709-1711
Published: June 15, 1971
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The equilibrium shift of the finite β fat-snake configurations with sharp plasma surfaces is calculated analytically and is found to be finite under the influence of the toroidal perturbation.
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Takashi Nagashima
1971 Volume 30 Issue 6 Pages
1712-1718
Published: June 15, 1971
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Spatial behaviours of electron plasma waves due to beam-plasma instability have been studied with a waveguide antenna which did not give any disturbance on the plasma. The observed growth rates are in agreement with those obtained by linear theory considering the plasma temperature. The criteria of validity of linear theory and the saturation of wave amplitude are also discussed. The electron beam modulated with microwave frequency gives rise to a strong electron plasma wave which shows the amplitude oscillation phenomena. The experimental value of its wave length agrees with the theoretical one on the order of magnitude. The modulation was applied to the beam. The intensity of waves showed a dip when the modulation frequency was varied near the receiving frequency.
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Yasuji Hamada
1971 Volume 30 Issue 6 Pages
1719-1721
Published: June 15, 1971
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In 0.2 μs after the large electric field up to 60 V/cm was induced electromagnetically on the toroidal plasma, it showed an anomalous resistivity and intense UHF and VHF bursts around 1⁄2(
M⁄
m)
1⁄6ω
pi up to 50 V
p-p were observed. The lower part of the frequency spectrum of plasma oscillations was ascribed to the Buneman Instability. Its dependence on the plasma density was observed and was in agreement with the theoretical predictions.
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Kunioki Mima, Kyoji Nishikawa
1971 Volume 30 Issue 6 Pages
1722-1733
Published: June 15, 1971
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A general formulation is developed to investigate the stability of a collisionless, one-dimensional plasma which sustains a large-amplitude, monochromatic electron plasma wave. A nonlinear dispersion relation is derived which governs the stability of a small-amplitude test wave. It is shown that untrapped electrons can produce a significant modification to the Kruer-Dawson-Sudan dispersion relation which was derived by considering only the effect of trapped electrons on the test wave. As an application a weak-coupling limit is considered. It is shown that in this limit waves can grow in the distinct wavenumber regions given by
|
Δk|=\sqrt2
n+1
kB(
n=0, 1, 2, …),
and |
Δk|<<
kB where
Δk is the difference of the wavenumbers of the test wave and the original large-amplitude wave and
kB the bounce frequency divided by the phase velocity of the large-amplitude wave. Various characteristics of the growing waves are obtained.
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Moon-Uhn Kim, Chung-Oh Lee, Chul-Soo Kim
1971 Volume 30 Issue 6 Pages
1734-1746
Published: June 15, 1971
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This study deals experimentally and theoretically with pumping of a slightly conducting thin liquid layer by means of a traveling electric potential-wave and with electrohydrodynamic stability problem for the flow, which has a linear velocity profile, bounded by a fixed wall and an infinitely extended insulating liquid. It is shown that the induction pumping is successful in getting the film Reynolds number of order of few hundreds and that the limitation on the uniform flow results from flow instability. The stability problem is solved asymptotically for large values of the Reynolds number. The neutral stability curves are presented in α vs
R plane; the critical Reynolds number and its corresponding wave number are found. The comparison of the theory with experimental data on the interface velocity of laminar flow, the voltage corresponding to the critical Reynolds number and the most unstable wave-length of the disturbance is proved to be satisfactory.
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Akira Yoshizawa
1971 Volume 30 Issue 6 Pages
1747-1751
Published: June 15, 1971
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The laminar viscous flow past a semi-infinite flat plate is studied by means of the second approximation of the Oseen-type successive approximation. The Navier-Stokes equations are reduced to an integral equation for the shear stress on the plate by substituting the exact Oseen solution into the parts of the Navier-Stokes equations neglected in the Oseen approximation. The integral equation is solved with the kernel approximated appropriately. The analytical expression for the shear stress on the plate is obtained.
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Hanako Kobayashi, Ikuji Tsujikawa, Yukio Nakamura, Jiil C. Bonner, Sim ...
1971 Volume 30 Issue 6 Pages
1752
Published: June 15, 1971
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Katsuyuki Iizawa, Hiroyasu Fukaya, Isao Kitamura, Hironari Yamada, Tos ...
1971 Volume 30 Issue 6 Pages
1753-1754
Published: June 15, 1971
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Akio Kanbayasi, Tomonao Miyadai, Hiromitsu Kondo, Syôhei Miyahar ...
1971 Volume 30 Issue 6 Pages
1754
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Kenzô Kai, Takurô Nakamichi
1971 Volume 30 Issue 6 Pages
1755
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Mitsugu Hanabusa
1971 Volume 30 Issue 6 Pages
1756
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Setsuo Kajiwara
1971 Volume 30 Issue 6 Pages
1757
Published: June 15, 1971
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Yukishige Kawasaki, Shozo Ino, Shiro Ogawa
1971 Volume 30 Issue 6 Pages
1758-1759
Published: June 15, 1971
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Hideo Takezoe, Ikuo Maruyama, Akira Yoshikawa, Akio Honma, Ryumyo Onak ...
1971 Volume 30 Issue 6 Pages
1759
Published: June 15, 1971
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S. C. Jain, K. S. K. Sai
1971 Volume 30 Issue 6 Pages
1760
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Motowo Tsukakoshi
1971 Volume 30 Issue 6 Pages
1761
Published: June 15, 1971
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Toshihiro Arai, Kunio Wakamura, Keiei Kudo
1971 Volume 30 Issue 6 Pages
1762
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Hiroshi Tamura, Taizo Masumi
1971 Volume 30 Issue 6 Pages
1763
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Makoto Watanabe, Kaizo Nakamura
1971 Volume 30 Issue 6 Pages
1764
Published: June 15, 1971
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Yasuhiro Kondo, Masamitsu Hirai
1971 Volume 30 Issue 6 Pages
1765
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Chikara Sugiura
1971 Volume 30 Issue 6 Pages
1766
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Naoshi Hishinuma, Taizo Sasaki
1971 Volume 30 Issue 6 Pages
1767
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Kiyoshi Hayase, Takayoshi Okuda
1971 Volume 30 Issue 6 Pages
1768
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Teiichiro Yagi, Tsuneyasu Kura
1971 Volume 30 Issue 6 Pages
1769
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Shigeo Hamada
1971 Volume 30 Issue 6 Pages
1770
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Osamu Matsuoka, Tosiyasu L. Kunii
1971 Volume 30 Issue 6 Pages
1771
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Takasuke Matsuo, Hiroshi Suga, Syûzô Seki
1971 Volume 30 Issue 6 Pages
1772
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