• 《常微分方程教程》习题2-2,4:一个跟踪问题


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     74 % ----------------------------------------------------------------------------------------
     75 %    TITLE
     76 % ----------------------------------------------------------------------------------------
     77 
     78 	itle{	extbf{《常微分方程教程》习题2-2,4\[2em]一个跟踪问题}} 
     79 
     80 author{small{叶卢庆}\{small{杭州师范大学理学院,学号:1002011005}}\{small{Email:h5411167@gmail.com}}} % Institution
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     84 % ----------------------------------------------------------------------------------------
     85 
     86 egin{document}
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     88 
     89 % ----------------------------------------------------------------------------------------
     90 %    ABSTRACT AND KEYWORDS
     91 % ----------------------------------------------------------------------------------------
     92 
     93 % 
    enewcommand{abstractname}{摘要} % Uncomment to change the name of the abstract to something else
     94 
     95 % egin{abstract}
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     99 % hspace*{3,6mm}	extit{关键词:}  % Keywords
    100 
    101 % vspace{30pt} % Some vertical space between the abstract and first section
    102 
    103 % ----------------------------------------------------------------------------------------
    104 %    ESSAY BODY
    105 % ----------------------------------------------------------------------------------------
    106 egin{exercise}[2-2,4]
    107 跟踪:设某 $A$ 从 $Oxy$  平面的原点出发,沿 $x$ 轴正方向前进;同时某 $B$
    108 从点 $(0,b)$ 开始跟踪 $A$,即 $B$ 的运动方向永远指向 $A$ 并与 $A$ 保持
    109 等距 $b$.试求 $B$ 的光滑运动轨迹.
    110 end{exercise}
    111 egin{proof}[解]
    112 设在时刻 $t$ 的时候 $A$ 位于 $(f(t),0)$.其中 $f(0)=0$,且 $f(t)$ 是关于
    113 $t$ 的严格单调增函数.设在时刻 $t$ 的
    114 $B$ 位于 $(P(t),Q(t))$,其中 $P(0)=0,Q(0)=b$.不妨设 $b
    eq 0$,否则 $B$
    115 的运动将与 $A$ 重合,这是没什么意思的,再根据对称性不妨设 $b>0$.且由于 $B$ 的路径光滑,因此关于
    116 $t$ 的函数 $P,Q$ 都是连续可微的.由于 $B$ 的方向一直指向 $A$,因此
    117 egin{equation}
    118   label{eq:10.51}
    119   (P'(t),Q'(t))=k(f(t)-P(t),-Q(t)).
    120 end{equation}
    121 其中 $k>0$.由于 $A,B$ 间距始终为 $b$,因此
    122 egin{equation}
    123   label{eq:10.52}
    124   [P(t)-f(t)]^2+Q(t)^2=b^2.
    125 end{equation}
    126 当 $Q(t)
    eq 0$ 时,$Q'(t)$ 也不为0.此时 将(1) 代入 (2) 可得
    127 egin{equation}
    128   label{eq:11.02}
    129   (P'(t))^2+(Q'(t))^2=b^2k^2=b^2frac{Q'(t)^{2}}{Q(t)^{2}}.
    130 end{equation}
    131 于是我们就得到了微分方程
    132 egin{equation}
    133   label{eq:11.54}
    134   (frac{P'(t)}{Q'(t)})^2+1=frac{b^2}{Q(t)^2}.
    135 end{equation}
    136 也就是
    137 $$
    138 (frac{dP(t)}{dQ(t)})^2+1=frac{b^2}{Q(t)^2}.
    139 $$
    140 也即
    141 $$
    142 frac{dx}{dy}=-sqrt{(frac{b}{y})^2-1}.
    143 $$
    144 令 $frac{b}{y}=cosh a$.其中 $ain mathbf{R}^{+}$,于是,
    145 $$
    146 frac{dy}{da}=frac{-b	anh a}{cosh a}.
    147 $$
    148 149 $$
    150 frac{dx}{dy}=-sinh a.
    151 $$
    152 因此,
    153 $$
    154 frac{dx}{da}=b(	anh a)^2=b-b	anh'a.
    155 $$
    156 因此,
    157 $$
    158 x=ba-b	anh a+C.
    159 $$
    160 因此,
    161 $$
    162 x=bcosh^{-1}frac{b}{y}-b	anh(cosh^{-1}frac{b}{y})+C.
    163 $$
    164 将初始条件 $x=0,y=b$ 代入,解得 $C=0$.于是 $B$ 的光滑轨迹为
    165 $$
    166 x=bcosh^{-1}frac{b}{y}-b	anh(cosh^{-1}frac{b}{y}).
    167 $$
    168 通过这个方程,我们发现 $B$ 的运动轨迹和 $A$ 的运动无关!\
    169 
    170 当 $Q(t)=0$ 时,易得 $B$ 已经和 $A$ 同在 $x$ 轴上运动.
    171 end{proof}
    172 % ----------------------------------------------------------------------------------------
    173 %    BIBLIOGRAPHY
    174 % ----------------------------------------------------------------------------------------
    175 
    176 ibliographystyle{unsrt}
    177 
    178 ibliography{sample}
    179 
    180 % ----------------------------------------------------------------------------------------
    181 end{document}
    View Code
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  • 原文地址:https://www.cnblogs.com/yeluqing/p/3827355.html
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