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161.
A shock tube was utilized for transdermal delivery in fuzzy rats. Rhodamine-B dextran, 10 kDa molecular weight, was used
as the probe molecule. Shock waves were generated by a two-stage shock tube. A single shock wave was applied onto the skin
to permeabilize the stratum corneum. Subsequently, the dextran solution diffused through the stratum corneum into the epidermis.
Fluorescence microscopy of biopsies showed that the dextran was delivered to a depth of m into the skin. Thus, the shock tube could become an inexpensive device for transdermal drug delivery.
Received 19 February 2000 / Accepted 29 June 2000 相似文献
162.
The pattern of shock wave reflection over a wedge is, in general, either a regular reflection or a Mach reflection, depending
on wedge angles, shock wave Mach numbers, and specific heat ratios of gases. However, regular and Mach reflections can coexist,
in particular, over a three-dimensional wedge surface, whose inclination angles locally vary normal to the direction of shock
propagation. This paper reports a result of diffuse double exposure holographic interferometric observations of shock wave
reflections over a skewed wedge surface placed in a 100 × 180 mm shock tube. The wedge consists of a straight generating line
whose local inclination angle varies continuously from 30° to 60°. Painting its surface with fluorescent spray paint and irradiating
its surface with a collimated object beam at a time interval of a few microseconds, we succeeded in visualizing three-dimensional
shock reflection over the skewed wedge surface. Experiments were performed at shock Mach numbers, 1.55, 2.02, and 2.53 in
air. From reconstructed holographic images, we estimated critical transition angles at these shock wave Mach numbers and found
that these were very close to those over straight wedges. This is attributable to the flow three-dimensionality.
相似文献
163.
Ivan Christov 《International Journal of Non》2009,44(5):511-519
We examine the propagation of shocks and traveling wave phenomena on a one-dimensional string that is executing finite-amplitude, transverse vibrations in a resisting medium. As part of our study, we develop an approach that allows us to describe, albeit approximately, the evolution and propagation of a shock front using analytical methods. In addition, exact traveling wave solutions, one of which involves the Lambert W-function, of the string's equation of motion are determined and analyzed. Lastly, a possible new form of the solution to the linearized problem is presented and extensions and other applications of the present work are briefly discussed. 相似文献
164.
An Efficient Method for Computing Hyperbolic Systems with Geometrical Source Terms Having Concentrations 总被引:3,自引:0,他引:3
ShiJin XinWen 《计算数学(英文版)》2004,22(2):230-249
We propose a simple numerical method for calculating both unsteady and steady state solution of hyperbolic system with geometrical source terms having concentrations. Physical problems under consideration include the shallow water equations with topography,and the quasi one-dimensional nozzle flows. We use the interface value, rather than the cell-averages, for the source terms, which results in a well-balanced scheme that can capture the steady state solution with a remarkable accuracy. This method approximates the source terms via the numerical fluxes produced by an (approximate) Riemann solver for the homogeneous hyperbolic systems with slight additional computation complexity using Newton‘s iterations and numerical integrations. This method solves well the subor super-critical flows, and with a transonic fix, also handles well the transonic flows over the concentration. Numerical examples provide strong evidence on the effectiveness of this new method for both unsteady and steady state calculations. 相似文献
165.
用吉布斯自由能最小原理,通过解化学平衡方程组,求解PETN炸药爆轰产物系统的平衡组分,计算结果与用BKW和LJD方法计算的结果相近.用自编的程序从碳的石墨相、金刚石相、类石墨液相和类金刚石液相4种相态中确定出炸药爆轰产物中游离碳更可能存在的相态,并用此相态计算碳的Gibbs自由能,以WCA状态方程作为爆轰气相产物的物态方程,对PETN炸药爆轰参数作了预言,爆轰CJ点的爆速、爆压和爆温的计算结果与实验值吻合得很好. 相似文献
166.
167.
168.
The interaction between fast shallow granular flow and obstacles on steep terrain is an important aspect of granular mechanics and defending against geological hazards. In this study, we used a depth-averaged model for granular flow facing obstacles on steep terrains in a bed-fitted coordinate system where the obstacle system is treated as a local bed deviation term. A second-order Riemann-free scheme is extended to compute the depth-averaged model with a wetting–drying technique, which is verified by several granular flow cases, such as aluminum bar collapse and granular flow runout on a steep slope. Numerical simulations were performed for the case of granular flow facing a (i) single hemispherical obstacle and (ii) system of three hemispherical obstacles to produce a dynamical process and deposit profile, and show good agreement with experimental results. Granular flow facing a single obstacle on a concave plane produces a detached shock wave that moves upstream and a tailing rapid transition zone that moves down, which will merge to form a new shock for deposition. Granular flows facing a three-hemisphere obstacle system produce a tailing rapid transition zone that moves downstream and a downstream wavy shock that results from the interaction of three bow shocks in front of each obstacle. The downstream wavy shock moves upstream and merges with the upstream transition zone to form a new curved shock, which later relaxes to a deposit owing to bed friction. These findings provide some supplemental understandings of flow structures of fast granular flow facing obstacles. 相似文献
169.
170.
B. M. Argrow 《Shock Waves》1996,6(4):241-248
Nonclassical phenomena associated with the classical dynamics of real gases in a conventional shock tube are studied. A TVD
predictor-corrector (TVD-MacCormack) scheme with reflective endwall boundary conditions is used for the one-dimensional Euler
equations to simulate the evolution of the wave field of a van der Waals gas. Depending upon the initial conditions of the
gas, wave fields are produced that contain nonclassical phenomena such as expansion shocks, composite waves, splitting shocks,
etc. In addition, the interactions of waves reflected from the endwalls produce both classical and nonclassical phenomena.
Wave field evolution is depicted using plots of the flow variables at specific times and withx-t diagrams. 相似文献