1. What's Geosciences 3. Reviews 3D Models 4. Objects of 3D Geosciences Modeling 5. Data Sources of 3DGM 6. Forelands of 3DGM 7. Principles of GTP Model 8. Applications of GTP-based Geomo3D

Color Atlas of Pharmacology 2nd edition, revised and expanded Heinz Lüllmann, M. D. Professor Emeritus Department of Pharmacology University of Kiel Germany Klaus Mohr, M. D. Professor Department of Pharmacology and Toxicology Institute of Pharmacy University of Bonn Germany Albrecht Ziegler, Ph. D. Professor Department of Pharmacology University of Kiel Germany Detlef Bieger, M. D. Professor Division of Basic Medical Sciences Faculty of Medicine Memorial University of Newfoundland St. John’s, Newfoundland Canada 164 color plates by Jürgen Wirth

1. Ich bin a)deine b)deiner c)deinem d)deinen 2. Habt ihr Aufenthaltserlaubnis schon beantragt? a)ihre b)Ihre c)euer d 3. Der D-Zug nicht in Koblenz a)halt b) halt c) haltet d)halten

(1)(2)B(3)D (4)D (5)B 6)b(7) (8)B (9)D(10)D (11)(12)B(13)B(14)C(15)A

一、FLAC3D软件简介 二、FLAC3D的基本原理 三、FLAC3D的前后处理 四、流-固耦合分析 五、接触单元与应用 六、完全非线性的动力分析 七、自定义本构模型的基本方法 八、结构单元及应用

In this lecture, we consider the motion of a 3D rigid body. We shall see that in the general three dimensional case, the angular velocity of the body can change in magnitude as well as in direction, and, as a consequence, the motion is considerably more complicated than that in two dimensions. Rotation About a Fixed Point We consider first the simplified situation in which the 3D body moves in such a way that there is always a point, O, which is fixed. It is clear that, in this case, the path of any point in the rigid body which is at a

一、选择题 1．（A） 2．（C） 3．（D） 4．（B） 5．（B） 6．（C） 7.（D） 8．（D） 9．（D） 10．（B）

11.1 概述 11.2 D/A转换器 11.3 A/D转换器

一、 有关D/A、A/D的基本概念 二、 DAC及其接口 三、 ADC及其接口 四、 A/D，D/A应用举例

In lecture D9, we saw the principle of impulse and momentum applied to particle motion. This principle was of particular importance when the applied forces were functions of time and when interactions between particles occurred over very short times, such as with impact forces. In this lecture, we extend these principles to two dimensional rigid body dynamics. Impulse and Momentum Equations Linear Momentum In lecture D18, we introduced the equations of motion for a two dimensional rigid body. The linear momen- tum for a system of particles is defined