共查询到20条相似文献,搜索用时 15 毫秒
1.
Anna Perelomova 《Central European Journal of Physics》2011,9(1):138-145
This study is devoted to the instantaneous acoustic heating of a Bingham plastic. The model of the Bingham plastic’s viscous
stress tensor includes the yield stress along with the shear viscosity, which differentiates a Bingham plastic from a viscous
Newtonian fluid. A special linear combination of the conservation equations in differential form makes it possible to reduce
all acoustic terms in the linear part of of the final equation governing acoustic heating, and to retain those belonging to
the thermal mode. The nonlinear terms of the final equation are a result of interaction between sounds and the thermal mode.
In the field of intense sound, the resulting nonlinear acoustic terms form a driving force for the heating. The final governing
dynamic equation of the thermal mode is valid in a weakly nonlinear flow. It is instantaneous, and does not imply that sounds
be periodic. The equations governing the dynamics of both sounds and the thermal mode depend on sign of the shear rate. An
example of the propagation of a bipolar initially acoustic pulse and the evolution of the heating induced by it is illustrated
and discussed. 相似文献
2.
Voronovich AG 《The Journal of the Acoustical Society of America》2008,123(5):2480-2483
When a "massless" one-dimensional sound pulse (mass of a sound pulse is defined as an integral of the perturbation of density over the pulse length) reflects from a pressure-release boundary, its momentum changes sign. This obviously violates momentum conservation. However, in contrast to the case of an unbounded medium, calculation of the momentum in a bounded region includes a second-order term as well. Apparently, the second-order correction to the linear solution ensures momentum conservation in this case. The purpose of this Letter is to find a concrete form of this second-order correction. It appears that, as a result of the nonlinear interaction of the pulse with a pressure-release boundary, the latter experiences second-order net shift. This leads to the generation of a massive second-order rarefaction pulse whose momentum is directed opposite to the direction of propagation of the pulse itself. Appearance of this pulse ensures total momentum conservation. 相似文献
3.
In the present paper the propagation property of nonlinear waves in a thin viscoelastic tube filled with incom-pressible inviscid fluid is studied.The tube is considered to be made of an incompressible isotropic viscoelastic material described by Kelvin-Voigt model.Using the mass conservation and the momentum theorem of the fluid and radial dynamic equilibrium of an element of the tube wall,a set of nonlinear partial differential equations governing the prop-agation of nonlinear pressure wave in the solid-liquid coupled system is obtained.In the long-wave approximation the nonlinear far-field equations can be derived employing the reductive perturbation technique (RPT).Selecting the expo-nent α of the perturbation parameter in Gardner-Morikawa transformation according to the order of viscous coefficient η,three kinds of evolution equations with soliton solution,i.e.Korteweg-de Vries (KdV)-Burgers,KdV and Burgers equations are deduced.By means of the method of traveling-wave solution and numerical calculation,the propagation properties of solitary waves corresponding with these evolution equations are analysed in detail.Finally,as a example of practical application,the propagation of pressure pulses in large blood vessels is discussed. 相似文献
4.
Treeby BE Jaros J Rendell AP Cox BT 《The Journal of the Acoustical Society of America》2012,131(6):4324-4336
The simulation of nonlinear ultrasound propagation through tissue realistic media has a wide range of practical applications. However, this is a computationally difficult problem due to the large size of the computational domain compared to the acoustic wavelength. Here, the k-space pseudospectral method is used to reduce the number of grid points required per wavelength for accurate simulations. The model is based on coupled first-order acoustic equations valid for nonlinear wave propagation in heterogeneous media with power law absorption. These are derived from the equations of fluid mechanics and include a pressure-density relation that incorporates the effects of nonlinearity, power law absorption, and medium heterogeneities. The additional terms accounting for convective nonlinearity and power law absorption are expressed as spatial gradients making them efficient to numerically encode. The governing equations are then discretized using a k-space pseudospectral technique in which the spatial gradients are computed using the Fourier-collocation method. This increases the accuracy of the gradient calculation and thus relaxes the requirement for dense computational grids compared to conventional finite difference methods. The accuracy and utility of the developed model is demonstrated via several numerical experiments, including the 3D simulation of the beam pattern from a clinical ultrasound probe. 相似文献
5.
回热器的热声直流模型及其效应研究 总被引:2,自引:0,他引:2
本文由基本的守恒方程出发,获得了能描述回热器存在声直流时的非线性动力学模型及由此而导致的非线性时均热力学效应。根据所得到的模型,考察了声直流对临界声功产生率温度梯度、回热器温度分布以及脉冲管制冷性能的影响。 相似文献
6.
7.
A certain class of nonlinear evolution equations of one space dimension which permits kink type solutions and includes one-dimensional time-dependent Ginzburg-Landau (TDGL) equations and certain nonlinear wave equations is studied in some strong coupling approximation where the problem can be reduced to the study of kink dynamics. A detailed study is presented for the case of TDGL equation with possible applications to the late stage kinetics of order-disorer phase transitions and spinodal decompositions. A special case of kink dynamics of nonlinear wave equations is found to reduce to the Toda lattice dynamics. A new conservation law for dissipative systems is found which corresponds to the momentum conservation law for wave equations. 相似文献
8.
V. V. Bryksin 《Technical Physics》1998,43(11):1269-1274
It is shown that three types of solitary acoustic waves can develop in anharmonic crystal lattices corresponding to the three branches of acoustic phonons. A system of three nonlinear Schrödinger equations is derived to describe this situation. For greatly different group velocities, the interaction between solitons reduces collisions between them. When the group velocities of the different acoustic modes in a lattice are close to one another, bound states of the corresponding types of solitary waves occur. Bound states of this sort are vector solitons, whose polarization varies along the pulse. If the transverse acoustic modes are degenerate in velocity, the situation is extremely similar to the propagation of pulses in optical fibers. 相似文献
9.
N. V. Ustinov 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,58(3):311-317
The hierarchy of integrable nonlinear equations associated with the quadratic
bundle is considered.
The expressions for the solution of linearization of these equations and
their conservation law in the terms of solutions of corresponding Lax pairs
are found.
It is shown for the first member of the hierarchy that the conservation law is
connected with the solution of linearized equation due to the Noether's
theorem.
The local hierarchy and three nonlocal ones of the infinitesimal symmetries
and conservation laws explicitly expressed through the variables of the
nonlinear equations are derived. 相似文献
10.
11.
When acoustic waves are scattered by random sound-speed fluctuations in a two-dimensional channel the energy is continually transferred between the propagating modes. In the multiple- scattering region the energy flux assumes an asymptotic form in which there is equal energy flux propagating in each mode. Here we shall make use of this well known result to show how to obtain an asymptotic form for a pulse of acoustic energy propagating in the channel. In the multiple-scattering region the speed of the acoustic waves in the pulse continually changes as the energy is transferred between the modes. The process is basically a diffusion process around the mean speed of propagation. We shall first show, using physical arguments, that the diffusion coefficient is proportional to the square root of the propagation distance times the mean free path of scattering. The theory governing the acoustic propagation in the channel is formulated in terms of modal coherence equations and we shall next give a brief review of the definitions of the coherence functions and a discussion of how the equations governing the propagation of the modal coherence functions are derived. We shall then show how the pulse shape and the relevant parameters may be obtained by solving the basic modal coherence equations at large propagation distances. 相似文献
12.
An integral conservation law for wave numbers is considered. In order to test the validity of the proposed conservation law, a complete solution for the reflection and transmission of an acoustic wave impinging normally on a material interface moving at a constant speed is derived. The agreement between the frequency condition thus deduced from the dynamic equations of motion and the frequency condition derived from the jump condition associated with the integral equation supports the proposed law as a true conservation law. Additional comparisons such as amplitude discontinuities and Snells' law in a moving media further confirm the stated proposition. Results are stated concerning frequency and wave number relations across a shock front as predicted by the proposed conservation law. 相似文献
13.
本文在热质和热子气概念的基础上建立了热子气的质量、动量、能量守恒方程.基于傅立叶导热定律求得了热子气粘性系数和粘性力的近似表达式.分析了傅立叶定律的物理意义:傅立叶定律是在忽略惯性力的条件下对热子气动量方程的近似.在极低温度或极高热流密度条件下傅立叶定律不再适用. 相似文献
14.
In this paper, the complex short pulse equation and the coupled complex short pulse equations that can describe the ultra-short pulse propagation in optical fibers are investigated. The two complex nonlinear models are turned into multi-component real models by proper transformations. Lie symmetries are obtained via the classical Lie group method, and the results for the coupled complex short pulse equations contain the existing results as particular cases. Based on the linearizing operator and adjoint linearizing operator for the two real systems, adjoint symmetries can be obtained. Explicit conservation laws are constructed using the symmetry/adjoint symmetry pair (SA) method. Relationships between the nonlinear self-adjointness method and the SA method are investigated. 相似文献
15.
Rowland DR 《Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics》1999,59(6):7141-7147
The swapping of power between the modes of cw waves in lossless nonlinear optical waveguides always admit two conserved quantities, the total power and one other, which is sometimes identified as a Hamiltonian. We show that a general formulation of this Hamiltonian is in fact the weak guidance limit for cw waves of a more general conservation law. We make the link between this more general conservation law and the conservation of "wave" momentum, where wave momentum is a combination of both real momentum and so-called pseudomomentum. This allows us to interpret the conserved Hamiltonian in physical terms. 相似文献
16.
Kenneth J. Chau Henri J. Lezec 《Applied Physics A: Materials Science & Processing》2011,105(2):267-281
Over a half-century ago, Balazs proposed a thought experiment to deduce the form of electromagnetic momentum in a lossless
and non-dispersive slab by imposing conservation of global momentum and system center-of-mass velocity after a pulse has traveled
through the slab. Here, we revisit the Balazs thought experiment by explicit calculations of momentum transfer and center-of-mass
displacement of a non-dispersive, positive-index slab of arbitrary complex permittivity and permeability using a set of postulates
consisting only of Maxwell’s equations, a generalized Lorentz force law, the Abraham form of the electromagnetic momentum
density, and conservation of both pulse and slab mass. In the case where the slab is lossless, we show that a pulse of arbitrary
shape incident onto the slab conserves both global momentum and system center-of-mass velocity, consistent with the starting
postulates of the Balazs thought experiment. In the case where the slab is lossy, we show, within the context of the above
postulates, that global momentum is always conserved and that system center-of-mass velocity is conserved only when mass transfer
from the pulse to the slab is described by an incremental pulse-mass-transfer model, proposed here, in which the pulse deposits
mass in the slab with a distribution corresponding to the instantaneous mass density profile of the pulse. 相似文献
17.
本文利用约化摄动方法,从非线性介质中的原始Maxwell方程出发,首次导出了纵向非均匀介质波导中超短光脉冲演化方程,给出了描述飞秒光脉冲波包演化方程的两种等价表达式。 相似文献
18.
Multi-symplectic variational integrators for nonlinear Schrdinger equations with variable coefficients
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In this paper, we propose a variational integrator for nonlinear Schrdinger equations with variable coefficients. It is shown that our variational integrator is naturally multi-symplectic. The discrete multi-symplectic structure of the integrator is presented by a multi-symplectic form formula that can be derived from the discrete Lagrangian boundary function. As two examples of nonlinear Schrdinger equations with variable coefficients, cubic nonlinear Schrdinger equations and Gross–Pitaevskii equations are extensively studied by the proposed integrator. Our numerical simulations demonstrate that the integrator is capable of preserving the mass, momentum, and energy conservation during time evolutions. Convergence tests are presented to verify that our integrator has second-order accuracy both in time and space. 相似文献
19.
首先利用高速摄影和压力传感器测量的方法, 对曲面反射式水下强声波脉冲的传播和聚焦过程进行了实验研究.实验研究发现, 椭球面反射罩在起到汇聚声能的作用的同时也将使得强声波脉冲在传播过程中形成负压区, 并由此而引发近场声传播通道上空化气泡群的产生. 在实验结果的基础上, 进一步利用基于Kirchhoff衍射定理的声传播模型和大振幅条件下的QX气泡运动方程, 对强声波脉冲负压区的形成原因及空化气泡的运动过程进行了数值计算和分析. 研究结果表明, 在焦前区, 源于反射罩内表面的"尾波"和出口处的"边缘波"在传播过程中将形成反射波中的负压区; 在焦后区, 源于反射罩顶点的"中心波"在传播过程中将形成反射波中的负压区. 在反射波作用下, 空化气泡体现出了"正压区受压缩并振荡, 负压区膨胀"的运动特点. 在反射波之后, 空化气泡将出现成长、坍缩和回弹等典型的物理过程. 研究结果对曲面反射式水下强声波传播物理规律的认识具有实际意义. 相似文献
20.
The construction and testing of short pulse (bipolar and unipolar) ultrasound transducers are discussed and several examples are analysed. Equations predicting the radiation field of the short pulse transducer are derived using a new approach. Agreement was obtained between the theoretical predictions and the experimentally measured field for one short pulse transducer. Some discrepancy was noted between the predicted pulse shapes and those observed experimentally. 相似文献