• 検索結果がありません。

つくばリポジトリ AS 34 2

N/A
N/A
Protected

Academic year: 2018

シェア "つくばリポジトリ AS 34 2"

Copied!
6
0
0

読み込み中.... (全文を見る)

全文

Loading

Table 1 Experimental values for different packing supports a
Fig. 2 Three-dimensional  representation  using  plates,  time,  and  pressure for a totally porous silica particle of 2-µm diameter.
Fig. 5 KPL surfaces of (a) 3-µm packings, (b) 5-µm packings, and (c)  monolithic column.

参照

関連したドキュメント

To obtain the optimal time decay rates of the higher-order derivatives of the solution, we can represent the spatial derivatives of the solutions to the equation U t = BU + G with

In this study, a new metering method is presented based on homogeneous and separated flow theory; the acceleration pressure drop and the friction pressure drop of Venturi

Kaplick´ y shows H¨ older continuity of velocity gradients and pressure for (1.1) with p ∈ [2, 4) under no slip boundary conditions. Based on the same structure of the proof and

An example of a length 4 highest weight category which is indecompos- able and Ringel self-dual, and whose standard modules are homogeneous, is the path algebra of the linear

The finite element method is used to simulate the variation of cavity pressure, cavity volume, mass flow rate, and the actuator velocity.. The finite element analysis is extended

We obtain a ‘stability estimate’ for strong solutions of the Navier–Stokes system, which is an L α -version, 1 < α < ∞ , of the estimate that Serrin [Se] used in

Keywords: Nonfixed termination time, optimal control problem, periodic boundary conditions, Schr¨odinger equation, blow up, minimum.. 2010 AMS subject classification numbers:

Based on sequential numerical results [28], Klawonn and Pavarino showed that the number of GMRES [39] iterations for the two-level additive Schwarz methods for symmetric