一、肉松 肉松是我国著名的特产,它是指瘦肉经高温煮制、炒制脱水等工艺精制而成的肌肉纤维蓬松成絮状或团粒 状的干熟肉制品。具有营养丰富、味美可口易消化、食用方便、易于贮藏等特点。根据所用原料、辅料 等不同有猪肉松、牛肉松、羊肉松、鸡肉松等:根据产地不同,我国有名的传统产品有太仓肉松、福建肉 松等

一、掌握数据绑定的基本概念 二、掌握 GridView控件的基本用法 教学重点: 一、显示数据表记录 二、对数据表进行分页、排序和选择 三、利用模板美化显示 四、显示记录中的图像

教学是在教育目的的规范下,由教师的 教”与学生的“学”共同组成的教育活动, 通过教学,学生在教师有目的、有计划的指 导下,积极、主动地掌握系统文化科学知识 和技能,发展能力、增强体质,陶冶美感, 形成一定的思想品德和个性。 教学的实质是以知识的传授为基础,促 进学生身心的健康发展

Lecture D32: Damped Free Vibration Spring-Dashpot-Mass System k Spring Force Fs =-kx, k>0 Dashpot Fd =-cx, c>0 Newton's Second Law (mx =EF) mx +cx+kx (Define)Natural Frequency wn=k/m,and

一、斯威齐模型 二、也称为折弯需求曲线模型。 三、由美国经济学家斯威齐于1939年提出。 四、用于解释一些寡头市场上的价格刚性现象

When the only force acting on a particle is always directed to- wards a fixed point, the motion is called central force motion. This type of motion is particularly relevant when studying the orbital movement of planets and satellites. The laws which gov- ern this motion were first postulated by Kepler and deduced from observation. In this lecture, we will see that these laws are a con- sequence of Newton's second law. An understanding of central

In this lecture, we will consider how to transfer from one orbit, or trajectory, to another. One of the assumptions that we shall make is that the velocity changes of the spacecraft, due to the propulsive effects, occur instantaneously. Although it obviously takes some time for the spacecraft to accelerate to the velocity of the new orbit, this assumption is reasonable when the burn time of the rocket is much smaller than the period of the orbit. In such cases, the Av required to do the maneuver is simply the difference between the

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

In this lecture, we will revisit the application of Newton's second law to a system of particles and derive some useful relationships expressing the conservation of angular momentum. Center of Mass Consider a system made up of n particles. A typical particle, i, has mass mi, and, at the instant considered, occupies the position Ti relative to a frame xyz. We can then define the center of mass, G, as the point

Inertial reference frames In the previous lecture, we derived an expression that related the accelerations observed using two reference frames, A and B, which are in relative motion with respect to each other. aA =aB+(aA/ B)'y'' 22 x (DA/ B) 'y'2'+ TA/B+ X TA/B). (1) Here, aA is the acceleration of particle A observed by one observer, and