7.1 z-Transform of a Discrete-Time Signal
离散时间信号的 z 变换
Z-Pair Explorer — z 变换对照表
Pick a canonical sequence and see four things in sync: the closed-form
, the region of convergence (ROC, shaded green),
the pole/zero map on the z-plane, and the time-domain stem.
选一种典型序列,可一键看到它的 解析式、
收敛域 ROC(绿色阴影)、z 平面零极点图与时域 stem。
对比第 3、4 项:解析式完全相同,但 ROC 不同, 也不同——
这正是 ROC 不可省略的原因。
s ↔ z Mapping —
Why is the z-plane "circular" while the s-plane is "flat"? Because
, with
. Drag the sliders to a point
in the s-plane and watch the image dot
in the z-plane. Every -shift of
brings you back to the same z —
this is the geometric origin of spectral aliasing.
s 平面上 每偏移 ,
z 平面上的像点回到同一位置;这就是谱混叠的几何根源。
Q1: Why do and share the same ?两个完全不同的 x[n] 为何对应相同的 X(z)?
The closed form is an analytic continuation of the geometric series. The algebraic identity is only meaningful inside a particular ROC: right-sided sums converge for ; left-sided sums converge for . So the pair (X(z), ROC) is what uniquely determines — not alone.
闭式 是几何级数的解析延拓—— 单独看代数表达式不可逆,必须配上 ROC:右边序列对应 , 左边序列对应 。
Q2: For a right-sided sequence, what does "pole inside / on / outside the unit circle" mean physically?右边序列的极点在单位圆内/上/外,分别意味着什么?
For a causal (right-sided) sequence, the ROC is "outside the outermost pole". The DTFT exists iff the unit circle lies inside the ROC, i.e. iff all poles are strictly inside the unit circle:
- Pole inside (): decaying sequence — stable, DTFT exists.
- Pole on (): marginally stable — bounded but not absolutely summable; DTFT exists only as a distribution (e.g. has a δ-spike at DC).
- Pole outside (): unbounded growth — unstable; no DTFT.
右边序列的 ROC 是"最外极点之外";要让 DTFT 存在,所有极点必须在单位圆内。 极点在圆上 = 临界稳定(u[n]、cosine 都是这种情况);极点在圆外 = 发散。
Q3: Why does the same z keep "appearing" when I slide Ω past 2π?为什么 Ω 每过 2π,z 平面上的点就重合?
Because is periodic in with period . Algebraically:
Geometrically: infinitely many horizontal strips of height in the s-plane all wrap onto the same z-plane circle. Continuous-time spectra repeat after sampling — this is the spectral aliasing of §4.2 viewed from the z side.
采样在频域引入 周期,所以 s 平面里宽 的水平条带都会被 映到同一圈 z。
Q4: Where do the poles of sit, and why?cos(Ω₀n)·u[n] 的极点为何落在单位圆上?
By Euler: . Each complex exponential is a special case of with — so its pole is at , exactly on the unit circle. The cosine is a sum of these two, giving conjugate poles on the unit circle at angles . Switching to retracts the poles inward to radius — a decaying oscillation.
复指数 的极点在 ,余弦 = 两个共轭复指数之和,所以共轭极点对落在单位圆上、辐角 ±Ω₀ 处。 a<1 时极点向原点缩,对应衰减振荡。
Q5: A finite-length pulse has poles only at the origin and zeros all around the unit circle. Why?有限长矩形脉冲的极点全在原点,零点为何均匀分布在单位圆上?
For on :
The numerator has roots at the -th roots of unity, but the root at cancels with the denominator's . The survivors are zeros evenly spaced on the unit circle at , and poles all at . ROC is "everywhere except " — finite-length sequences have essentially the entire z-plane as ROC.
长度 L 的矩形脉冲是几何级数和:分子 z^L−1 的 L 个根中去掉与分母约掉的 z=1,剩下 L−1 个零点均匀分布在单位圆上;极点全在原点。ROC = 整个 z 平面(除 0 外)。