一、磁场能量及能量密度 1、电磁能定域于场中 (1)电能定域于电场中,即场具有能量、电能储于电场中:w=d (2)同样,磁能也储于磁场中,场能密度为:Wm=B.H

3-3设某恒参信道可用图P3-1所示的线性二端口网络来等效。试求它的传输函数 H(w),并说明信号通过该信道时会产生哪些失真

Review Fundamentals of multibody dynamics Newton-Euler equation I;=-×工+n+nF =fw+ff Rely on free-body diagram. Constraint force involved Compact form m ti=-WiMti+w+wf

如果在晶体中存在温度梯度 w能流密度:0=-d一单位时间内通过单位面积的热能,其中为品体的热导系数。 不考虑电子对热传导的贡献,晶体中的热传导主要依靠声子来完成 当样品中存在温度梯度时,“声子气体”的密度分布是不均匀的。温度较高的区域将有产生较多的振 动模式和具有较大的振动幅度,即有较多的声子被激发,“声子”密度高。这些声子通过和晶体中其 它声子发生碰撞,使得温度较低的区域具有同样的“声子”密度

粘性流体运动的基本方程组 研究粘性流体运动问题时,我们关心的 物理量一般为: 流体的速度V, (对于空间流动,有u,V,w三速度分量) 以及三个热力学状态参数: 压强P,密度p和温度T

边界条件 At y-D: u=ue T-Te 上界流体和与动平板间的摩擦剪力τe 热传导qe Paralel streamline。 At y=0: u=0.T=Tw 下界流体和与动平板间的摩擦剪力τw 热传导qw

The hyde school In 1966, Joseph W. Gauld founded the first Hyde school in Bath, Maine in response to a system of education which hebelieved was failing its children because of conflicting priorities. His search for a new approach in education led to a program that valued attitude over aptitude, effort over ability, and s character over talent

Chapter 3 Transport Layer Computer Networking The Powerpoint slides are based on the A Top Down Approach material provided by Featuring the Internet J F Kurose and K.W. Ross 2nd edition

Chapter 7 Network Security Computer Networking A Top Down Approach Featuring the Internet, The power Point slides are based on the 2nd edition material provided by Jim Kurose, Keith Ross Lf Kurose and K.w. ross Addison-Wesley, July

3-11某APD管用于波长1.55μm,其平均雪崩增益为20,响应度为0.6A/W,当每秒钟有 1000个光子入射时,计算其量子效率和输出光电流