Tìm thấy 20+ kết quả cho từ khóa "Boundary conditions"
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The classical equations of the motion and the boundary conditions for the open rigid string follow from the requirement. for the any variation δx µ obeying following conditions. (11b) This conditions (11b) is due to the fact that Lagrangian contains the second order derivatives with respect to the evolution τ . Now, it is clear that the requirement (10) implies the following equations of motion. and the following boundary conditions.
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Uses of zeta regularization in QFT with boundary conditions: a cosmo-topological Casimir effect
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The norm of the function y(x. 0 | dx df | 2 dx by virtue of the boundary conditions on f. by virtue of the boundary conditions on f. n , the eigenvalues of the integral operators are 1. Some of the important operators and the properties of their eigenvalues. Because of the idealization,. C/m 3 (2.139a) where l is the linear density of the source. n (x) of the homogeneous differential equation corresponding to (2.129).
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Generally, sound pressure has to satisfy the sound wave equation (a second order Partial Differential Equation) and initial conditions of sound sources and boundary conditions of medium [1].. According to Normal mode (NM) theory [1-3], the sound pressure at the receiver is a summation of all propagation modes in space.
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The problems of natural vibration and forced vibration of a plate with various boundary conditions are studied. Effects of factors as geometry dimensions, order of laminate as well as waved-amplitude on frequency of natural vibration, amplitude of forced vibration of the corrugated cross-ply laminated composite plates are also analysed..
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Along with lack of an upper growth restriction of the nonlinearity and various boundary type conditions, the technicalities are more involved and different from two previous chapters. For the reaction-diffusion equations involving fractional Laplacian with extended Dirichlet boundary conditions and lack of an upper growth restriction of the non- linearity, we have the results by C.
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This bulk model is constructed with 3000 atoms (1000 Si atoms and 2000 O atoms) at temperatures 300K, 500K, 1000K, 1500K, 2000K, 2500K, 3000K and 3500K and at the pressure 0GPa by the Molecular Dynamics Simulation method with the van Beest-Kramer-van Santen (BKS) pair interaction potential and periodic boundary conditions. When the temperature was increased, the number of samples with the coordination number 4 decreased while number of samples with the coordination number 5 and 6 increased..
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The phase boundary of the superconducting disk (Fig. It should be emphasized that the presence of the oscillations in the H c3 (T ) curve is crucially dependent on the im- posed Neumann boundary conditions [45]. to the penetration of the first flux line [45]:. Even deeper in the superconducting area, the recovery of the normal Φ 0. The precise shape of the T c (H ) curve crucially depends on the area fraction for which T c (H ) 6 = 0..
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Thirdly, all of the suggested criteria have to meet the demand of boundary conditions. Many farmers now are already in debt because of the loans they took for their initial investment costs. Effect on diseases: if polluted substances in the water are reduced to the needed or desired water quality standards, the . Environmental impact: measures can be taken at the intake or outlet of the shrimp farms.
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CAMUS mockup – Description of the test Boundary conditions Fixed base Scale 1/3 Height/Length ≈3 Walls (l/h/d) m Floors (l/l/d) m 1.7x5.1x0.06 Base slab (l/h/d) m 1.7x1.7x0.21 Normal stress at the base MPa 1.7x0.6x0.06 Masse Kg 1.6 FIG. CAMUS mock-up Numerical Analysis Calibration A measure on the original structure of the eigenfrequencies before testing helped us to adjust and calibrate the model in terms of boundary conditions stiffness.
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Equivalently, it can be represented by boundary conditions of the form. In each of the regions (inside and outside), we can write. For each of the four. The Hamiltonian of the two-level atom is simply.
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A sin kx) 0 dx 1 So we can start applying boundary conditions: L x=0 ψ=0 x sin 2kx 2 0 A sin 0k B cos 0k 0 0 B *1 B 0 A. II sin Born Interpretation II. 6 1010 m. Molecular structure, realistic potential give accurate calculation, but It is the mass and size alone that set scale.
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If governing equations in a Cartesian system are directly used to flow past complex geometry, the imposition of boundary conditions will require a complicated interpolation of the data on local grid lines since the computational boundaries of complex geometry do not coincide with coordinate lines. This leads to a local loss of accuracy in the computed solutions.
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Restricting ourselves in the 1-D time-independent SEQ. substitute U(x) in the Schrödinger equation. identify the boundary conditions for wave function (x). A potential well is of the following form:. move in the 1-D box, and have any energy (a continuum od energy levels).. The time independent SEQ for the region 0 <. These are the wave functions which describe the states of a particle in the 1-D potential well.
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Just the absence of the quark and gluon states in the left-hand side Eq.(1) is called the confinement hypothesis.. n f is the number of flavours of quarks, Λ is the infrared boundary conditions for solutions of the renormalizable equation. Attempts are made to bind Λ with the scale of the P CAC and hadron mass spectra..
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In fact this coincides with the location of the horizon of the AdS black hole.. (13.2.10) The appropriate boundary conditions are φ → 0 at the boundary of the AdS, i.e. (14.0.2) where X i run over the coordinates in the plane of the horizon.We will refer to X i as the transverse coordinates, because they are transverse to the direction of motion of the point particle.The trajectory of the particle is taken to be. coordinates with X + playing the role of the independent time coordinate.. e 1 (σ 1
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Remark 1.9: The boundary conditions on the surface between two different media can be easily obtained from (1.31) and (1.32), and they are. and the details of the physical phenomena occurring on an atomic scale can be ignored. is also a solution of the linear equation. where v is the velocity of the particle. Let E 1 , H 1 and E 2 , H 2 be two solutions of the time-harmonic Maxwell equations. By the analyticity of the electromagnetic fields, one must have E = H = 0 in the region V .
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The treatment of the Penrose process in Sec. and (2) the justification of the boundary conditions used in the super-radiant interval. And there was the matter of the Prologue. THE PERTURBATIONS OF THE SCHWARZSCHILD METRIC 1. The Instability of the Inner Horizon VII. The uniqueness of the Kerr Metric 5. A General Description of the Geodesies 4. THE PERTURBATIONS OF THE KERR METRIC I:. THE PERTURBATIONS OF THE KERR METRIC II:. The Reduction of the Equations 2. Summary of the Solution 7.
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Dirichlet boundary conditions, if the ends of the string are held fixed.. of the other brane, forming an n -dimensional lattice. One of the two branes (for instance, the antibrane D 3 ) is frozen at a fixed position. was moving over the face of the waters
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At four sides of the computation domain, radiation boundary conditions are used in order to allow waves to go freely through the side boundary. A solitary wave is generated as the initial condition at a line parallel with the y direction, and located at the distance of 12.96 m from the center of the island. where x s is the center of the solitary wave.