\documentclass[14pt,a4paper,oneside]{extarticle}
\usepackage[left=30mm,right=15mm,top=20mm,bottom=20mm,bindingoffset=0mm]{geometry}
\setcounter{page}{2}
\renewcommand{\baselinestretch}{1.5}
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\usepackage[english,russian]{babel}
\usepackage{textcomp,latexsym,amsfonts,amsthm,amsmath,pifont,amssymb}
\usepackage{graphicx}
\usepackage{float}
\usepackage{amsmath}
\usepackage{colortbl}
%usepackage{setspace}
\usepackage{multicol}
\usepackage{indentfirst}
%usepackage{ccaption}
\usepackage{tocloft}
\usepackage{caption}
%captiondelim{. }
\setlength{\parindent}{1.25cm}
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\renewcommand{\thesubsection}{\arabic{section}.\arabic{subsection}.}
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#1\nobreak\cftdotfill{\cftdotsep} #2\par
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format=CustomTable,
font={normalsize},
labelformat=fullparents,
labelsep=fill,
justification=centering,
singlelinecheck=false,
skip=0pt
}
\theoremstyle{definition}
\newtheorem{definition}{Определение}
\newtheorem{theorem}{Теорема}
\newtheorem{proposition}{Следствие}
\newtheorem{lemma}{Лемма}
\sloppy
\begin{document}
\textbf{Решение}
\begin{enumerate}
\item Гамильтониан: $H = \psi_1 v + \psi_2 (\frac{uF}{M} - g)$
\item Уравнения Эйлера-Лагранжа:
\begin{multicols}{3}
\[
\begin{cases}
\psi^{\prime}_1 = -\frac{\partial H}{\partial h}\\
\psi^{\prime}_2 = -\frac{\partial H}{\partial v}\\
\end{cases}
\]
\columnbreak
\[
\begin{cases}
\psi^{\prime}_1 = 0\\
\psi^{\prime}_2 = -\psi_1\\
\end{cases}
\]
\columnbreak
\[
\begin{cases}
\psi_1 = C_1\\
\psi_2 = -C_1 t + C_2\\
\end{cases}
\]
\end{multicols}
\item Условие принципа максимума Понтрягина:
$$maxH = max(\psi_1 v + \psi_2 (\frac{uF}{M} - g)) = \psi_1 v - \psi_2 g + max(\psi_2\frac{uF}{M})$$
\end{enumerate}
\end{document}
我如何从顶部消除这个偏移?
答案1
您的最小工作示例不完整。尽管如此,我还是设法重现了错误。您必须\noindent
在第一列的开头添加一个。
在我看来,通过 multicol 的方式相当不方便。因此,我把所有这些都简单地放到了 parboxes 中
\begin{enumerate}
\item DEF: $H = \psi_1 v + \psi_2 (\frac{uF}{M} - g)$
\item 123 456:\\
\parbox[c]{0.4\linewidth}{
\[
\begin{cases}
\psi^{\prime}_1 = - \frac{\partial H}{\partial h}\\ \psi^{\prime}_2 = - \frac{\partial H}{\partial v} \end{cases}
\]
}\parbox[c]{0.3\linewidth}{
\[
\begin{cases} \psi^{\prime}_1 = 0\\ \psi^{\prime}_2 = -\psi_1
\end{cases} \]
}\parbox[c]{0.3\linewidth}{
\[
\begin{cases} \psi_1 = C_1\\ \psi_2 = -C_1 t + C_2
\end{cases} \]
}%parbox
\item GHI JKL MNO PQR: $$maxH = max(\psi_1 v + \psi_2 (\frac{uF}{M} - g)) = \psi_1 v - \psi_2 g + max(\psi_2\frac{uF}{M})$$
\end{enumerate}
答案2
您不需要multicols
环境parbox
。只需在一行中写入方程式,并\qquad
在其间留出间隙cases
:
\documentclass[12pt, a4paper]{extarticle}
\usepackage{mathtools}
\usepackage{enumitem}
\begin{document}
\begin{enumerate}
\item DEF: $H = \psi_1 v + \psi_2 (\frac{uF}{M} - g)$
\item 123 456:\\
\[
\begin{cases}
\psi^{\prime}_1 = - \frac{\partial H}{\partial h}\\
\psi^{\prime}_2 = - \frac{\partial H}{\partial v}
\end{cases}
\qquad
\begin{cases}
\psi^{\prime}_1 = 0\\
\psi^{\prime}_2 = -\psi_1
\end{cases}
\qquad
\begin{cases}
\psi_1 = C_1\\
\psi_2 = -C_1 t + C_2
\end{cases}
\]
\item GHI JKL MNO PQR:
\[
\max{H} = \max(\psi_1 v + \psi_2 \biggl(\frac{uF}{M} - g)\biggr)
= \psi_1 v - \psi_2 g + \max\biggl(\psi_2\frac{uF}{M}\biggr)
\]
\end{enumerate}
\end{document}
在上面的 MWE 中,我纠正了最后一个等式,因为我认为它应该正确写出。