在实际应用中,常常需要考察某种物理量(如温度,密度,电场 强度,力,速度等)在空间的分布和变化规律,从数学和物理上看这 就是场的概念。 设cR3是一个区域,若在时刻t,2中每一点(x,y,z)都有一个确 定的数值f(x,y,z,t)(或确定的向量值f(x,y,z)与它对应,就称函数 f(x,y,z,t)为2上的数量场(或向量场)

Problem set SolutioN Exercise for home study o&W8.35 (a) From the system diagram, we see that a(t)=a(t)cos(wet) Using the multiplication property ZGu)= o(X(u)* FT(cos wct)) FT of cos wt is two impulses with area T at +wc. Therefore, Z(w)is the spectrum

空间曲线的切线和法平面 一条空间曲线可以看成一个质点在空间运动的轨迹。取定一个直 角坐标系,设质点在时刻t位于点P(x()y()=(t)处,即它在任一时刻 的坐标可用 (x=x(t)

高阶导数的实际背景及定义 物体在时刻t的瞬时加速度为当t→0时,它的平均加速度的 △t 极限值,即

第一节树的类型定义 A为“根 T1、T2和T3都是一棵树,称为A的子树 称根和子树根之间的连线为“分支” 结点分支的个数定义为“结点的度”,如结点 B的度为2,D的度为3

Exercise for home study O&W4.47 tea this problem examines the Fourier transform of a continuous-time LTI system with a real, causal impulse response, h(t) (a) To prove that H(w) is completely specified by eh(u) for a real and causal h(t) lore the even part of a function, he(t)

Definition A real-valued function V: X H R defined on state space X of a system with behavior set B and state r:B×[0,∞)→ X is called a Lyapunov function if tHv(t)=v(a(t))=v(a(z(), t)) is a non-increasing function of time for every z E B according to this definition, Lyapunov

Fouriers derivation of the ct fourier transform x(t)-an aperiodic signal view it as the limit of a periodic signal as t→∞ For a periodic signal the harmonic components are spaced Oo=2π/ T apart. AsT→∞,Obo→>0, and harmonic components are space

Another(important! ) example: Periodic Impulse train n(t)=∑(t Sampling function important for sampling .2T

第一章第一构造定理 51.1.引言 设X(a)={x(t,a),t<()}是定义在完备概率空间(,F,P)上的齐次可列马尔可夫过程.其最小状态空间=(1,2,…),其转移概率矩阵(p(t),i1∈E是标准的,且其矩阵满足关系: