From 4ebf80ee3a25ae020bc9dc536614b815f47a162f Mon Sep 17 00:00:00 2001 From: Josh Gao Date: Thu, 20 Apr 2023 00:50:40 +0800 Subject: [PATCH] new post, josh-oap-1-2 --- source/_posts/2023-04-18-josh-oap-part-1-1.md | 2 + source/_posts/2023-04-20-josh-opa-part-1-2.md | 66 +++++++++++++++++++ 2 files changed, 68 insertions(+) create mode 100644 source/_posts/2023-04-20-josh-opa-part-1-2.md diff --git a/source/_posts/2023-04-18-josh-oap-part-1-1.md b/source/_posts/2023-04-18-josh-oap-part-1-1.md index 208ea62..dc9ad3a 100644 --- a/source/_posts/2023-04-18-josh-oap-part-1-1.md +++ b/source/_posts/2023-04-18-josh-oap-part-1-1.md @@ -217,6 +217,8 @@ $$\begin{equation} 定义 + + $$\begin{equation} \label{DefinitionOfArrayManifoldVector} \vec{v}_{\vec{k}}\left(\vec{k}\right) = \left[ \begin{array}{c} e^{-j \vec{k}^\mathrm{T}\vec{p}_0} \\ diff --git a/source/_posts/2023-04-20-josh-opa-part-1-2.md b/source/_posts/2023-04-20-josh-opa-part-1-2.md new file mode 100644 index 0000000..344f5d6 --- /dev/null +++ b/source/_posts/2023-04-20-josh-opa-part-1-2.md @@ -0,0 +1,66 @@ +--- +title: 'Josh''s Notes: 最优阵列处理(Part 1.2 —— 均匀线阵模型)' +mathjax: true +comments: true +copyright: true +toc: + enable: false + number: true + wrap: true + expand_all: true + max_depth: 4 +tags: + - 阵列信号处理 + - 均匀线阵 + - ULA +categories: + - - Josh 的学习笔记 + - 最优阵列处理 + - 阵列和空域滤波器 +abbrlink: de20fd09 +date: 2023-04-20 00:14:31 +--- + +我们感兴趣的线阵如[图 1-2-1](#fig.1-2-1) 所示,其中有 $N$ 个位于 $z$ 轴上的阵元,阵元间距均匀,记为 $d$。我们把这种阵列称为**{% label primary @均匀线性阵列(uniform linear array, ULA) %}**。我们已经把阵列的中心放在了坐标系的原点上,这种阵列中心放置方法将在计算量上具有优点。 + + + +![图 1-2-1 放置在 $z$ 轴上的线阵](https://josh-blog-1257563604.cos.ap-beijing.myqcloud.com/img/2023-04-20-josh-opa-part-1-2/2023-04-20-josh-oap-part-1-2-010-LinearArrayAlongZAaxis.png!sign){width=600px} + + + +  阵元的位置为 + +$$\begin{equation} \label{ElementLocation} +\begin{cases} + p_{x_n} = 0 \\ + p_{y_n} = 0 \\ + p_{z_n} = \left( n - \displaystyle\frac{N-1}{2} \right) d +\end{cases} + , \, n = 0,1,\cdots,N-1 +\end{equation}$$ + +为了确定阵列流形矢量 $\vec{v}_{\vec{k}}\left(\vec{k}\right)$, 把式 $\eqref{ElementLocation}$ 代入到[阵列流形矢量的定义][], 得到 + +$$\begin{equation} + \vec{v}_{\vec{k}}\left(k_z\right) = \left[\begin{array}{c} + e^{j \left( \frac{N-1}{2} \right) k_z d} \\ + e^{j \left( \frac{N-1}{2} - 1\right) k_z d} \\ + \vdots \\ + e^{-j \left( \frac{N-1}{2} \right) k_z d} \\ + \end{array}\right] +\end{equation}$$ + +这里 + +$$\begin{equation} + k_z = -\frac{2\pi}{\lambda}\cos\theta = -k_0 \cos\theta +\end{equation}$$ + +其中波数的幅度 + +$$\begin{equation} + k_0 \triangleq \left| \vec{k} \right| = \frac{2\pi}{\lambda} +\end{equation}$$ + +[阵列流形矢量的定义]: https://josh-gao.top/posts/8b61f5a7.html#DefinitionOfArrayManifoldVector