![格式化方程式](https://linux22.com/image/270145/%E6%A0%BC%E5%BC%8F%E5%8C%96%E6%96%B9%E7%A8%8B%E5%BC%8F.png)
\begin{align} \frac{1}{2} (1-\varepsilon^2)\left(\partial_\tau \phi\right)^2
= \frac{1}{2} \left(1-\epsilon ^2\right) \left(
-\frac{S \epsilon \sin\tau }{\sqrt{\lambda }}
-\frac{\text{g2} S^2 \epsilon ^2\sin2\tau }{3 \lambda }
+\epsilon ^3 \left(-\frac{\left(-\frac{1}{54} \text{g2}^2 S
\left(32+19 S^2\right) \lambda +Z \left(
\frac{35 \text{g2}^4}{27}
-\frac{7 \text{g2} \text{g4}}{4}+\frac{5 \text{g5}}{8}
-\frac{\text{g2}^2 \lambda }{6}
+\frac{\lambda ^2}{24}\right)\right) \sin\tau }{\lambda ^{5/2}}
-\frac{S^3 \left(4 \text{g2}^2-3 \lambda \right) \sin3\tau }
{24 \lambda ^{3/2}}\right)\right)^2
\end{align}
我想拆分 latex 文件中的方程式,我已经使用过, &
\qquad
但由于括号问题,它不起作用。我还能做什么?
答案1
在换行之前\left(
用 an关闭打开的文本,然后用\right.
\left.
答案如下:
\begin{align*} \frac{1}{2} (1-\varepsilon^2)\left(\partial_\tau \phi\right)^2
&= \frac{1}{2} \left(1-\epsilon ^2\right)\left(
-\frac{S \epsilon \sin\tau }{\sqrt{\lambda }}
-\frac{\text{g2} S^2 \epsilon ^2\sin2\tau }{3 \lambda }\right.\\
&\quad\left. +\epsilon ^3 \left(-\frac{\left(-\frac{1}{54} \text{g2}^2 S
\left(32+19 S^2\right) \lambda +Z \left(
\frac{35 \text{g2}^4}{27}
-\frac{7 \text{g2} \text{g4}}{4}+\frac{5 \text{g5}}{8}
-\frac{\text{g2}^2 \lambda }{6}
+\frac{\lambda ^2}{24}\right)\right) \sin\tau }
{\lambda ^{5/2}}\right.\right.\\
&\quad\left.\left.-\frac{S^3 \left(4 \text{g2}^2-3 \lambda \right) \sin3\tau }
{24 \lambda ^{3/2}}\right)\right)^2
\end{align*}
答案2
\left(
\right)
用(比如说)替换每一个\Bigl(
\Bigr)
如果您以这种方式手动选择大小,那么您可以将括号拆分到行和对齐单元格上。
此外,请始终发布完整的文档,而不仅仅是片段:
\documentclass{article}
\usepackage{amsmath}
\begin{document}
\begin{align*} \frac{1}{2} (1-\varepsilon^2)(\partial_\tau \phi)^2
&= \frac{1}{2} (1-\epsilon ^2) \Biggl(
-\frac{S \epsilon \sin\tau }{\sqrt{\lambda }}
-\frac{\text{g2} S^2 \epsilon ^2\sin2\tau }{3 \lambda }\\
&\quad +\epsilon ^3 \Bigl(-\frac{\Bigl(-\frac{1}{54} \text{g2}^2 S
(32+19 S^2) \lambda +Z \Bigl(
\frac{35 \text{g2}^4}{27}
-\frac{7 \text{g2} \text{g4}}{4}+\frac{5 \text{g5}}{8}
-\frac{\text{g2}^2 \lambda }{6}
+\frac{\lambda ^2}{24}\Bigr)\Bigr) \sin\tau }{\lambda ^{5/2}}\\
&\qquad -\frac{S^3 (4 \text{g2}^2-3 \lambda) \sin3\tau }
{24 \lambda ^{3/2}}\Bigr)\Biggr)^2
\end{align*}
\end{document}
答案3
\left
由于某种原因,您想将三条线居中。然后您可以执行以下操作(观察带有和 的注释版本\right
):
\documentclass{article}
\usepackage{amsmath}
\begin{document}
\[
\begin{array}{c}
\displaystyle
\frac{1}{2} (1-\varepsilon^2)
\left(
\partial_\tau \phi\right)^2
= \frac{1}{2} \left(1-\epsilon ^2\right)
%\left(
\Biggl(
-\frac{S \epsilon \sin\tau }{\sqrt{\lambda }}
-\frac{\text{g2} S^2 \epsilon ^2\sin2\tau }{3 \lambda }
%\right.
\\
\displaystyle
+\epsilon ^3
% \left(
\Biggl(
-\frac{\left(-\frac{1}{54} \text{g2}^2 S
\left(32+19 S^2\right) \lambda +Z \left(
\frac{35 \text{g2}^4}{27}
-\frac{7 \text{g2} \text{g4}}{4}+\frac{5 \text{g5}}{8}
-\frac{\text{g2}^2 \lambda }{6}
+\frac{\lambda ^2}{24}\right)\right) \sin\tau }{\lambda ^{5/2}}
%\right.
\\
\displaystyle
%\left.\left.
-\frac{S^3 \left(4 \text{g2}^2-3 \lambda \right) \sin3\tau }
{24 \lambda ^{3/2}}
%\right)\right)^2
\Biggr)\Biggr)^2
\end{array}
\]
\end{document}