2025 年考研数学二真题解析
2025 年全国硕士研究生招生考试
数学(二)
科目代码:302
考生注意事项
- 答题前,考生须在答题卡指定位置上填写考生编号和考生姓名;在答题卡指定位置上填写报考单位、考生姓名和考生编号,并涂写考生编号信息点.
- 选择题的答案必须涂写在答题卡相应题号的选项上,非选择题的答案必须书写在答题卡指定位置的边框区域内.超出答题区域书写的答案无效;在草稿纸、试题册上答题无效.
- 填(书)写部分必须使用黑色字迹签字笔书写,字迹工整、笔记清楚;涂写部分必须使用 2B 铅笔填涂.
- 考试结束,将答题卡和试题册按规定交回.
一、选择题
第 1~10 小题,每小题 5 分,共 50 分.下列每题给出的四个选项中,只有一个选项是符合题目要求的.
1
设函数 \(z=z\left( x,y \right)\) 由 \(z+\ln z-\int_{y}^{x} e^{-t^{2}} \mathrm{~d} t=0\) 确定,则 \(\dfrac{\partial z}{\partial x}+\dfrac{\partial z}{\partial y}=\)
A. \(\dfrac{z}{z+1}\left( e^{-x^{2}}-e^{-y^{2}} \right)\)
B. \(\dfrac{z}{z+1}\left( e^{-x^{2}}+e^{-y^{2}} \right)\)
C. \(-\dfrac{z}{z+1}\left( e^{-x^{2}}-e^{-y^{2}} \right)\)
D. \(-\dfrac{z}{z+1}\left( e^{-x^{2}}+e^{-y^{2}} \right)\)
答案:A
解析:
Note
本题更专业详细的解析(包含图示、相关知识详解,以及多种解法)请点击这里查看。
原式两边对 \(x\) 求导得 \(\dfrac{\partial z}{\partial x}+\dfrac{1}{z}\dfrac{\partial z}{\partial x}-e^{-x^{2}}=0\).
原式两边对 \(y\) 求导得 \(\dfrac{\partial z}{\partial y}+\dfrac{1}{z}\dfrac{\partial z}{\partial y}+e^{-y^{2}}=0\).
两式相加得 \(\dfrac{\partial z}{\partial x}+\dfrac{\partial z}{\partial y}=\dfrac{z}{z+1}\left( e^{-x^{2}}-e^{-y^{2}} \right)\).
2
已知函数 \(f\left( x \right)=\int_{0}^{x} e^{t^{2}}\sin t \mathrm{~d} t\),\(g\left( x \right)=\int_{0}^{x} e^{t^{2}} \mathrm{~d} t \cdot \sin^{2} x\),则
A. \(x=0\) 是 \(f\left( x \right)\) 的极值点,也是 \(g\left( x \right)\) 的极值点.
B. \(x=0\) 是 \(f\left( x \right)\) 的极值点,\(\left( 0,0 \right)\) 是曲线 \(y=g\left( x \right)\) 的拐点.
C. \(x=0\) 是 \(f\left( x \right)\) 的极值点,\(\left( 0,0 \right)\) 是曲线 \(y=f\left( x \right)\) 的拐点.
D. \(\left( 0,0 \right)\) 是曲线 \(y=f\left( x \right)\) 的拐点,也是曲线 \(y=g\left( x \right)\) 的拐点.
答案:B
解析:
\(f^{\prime}\left( x \right)=e^{x^{2}}\sin x\),\(f^{\prime\prime}\left( x \right)=e^{x^{2}}\cdot 2x\sin x+e^{x^{2}}\cos x\).
\(g^{\prime}\left( x \right)=e^{x^{2}}\sin^{3} x+\int_{0}^{x} e^{t^{2}} \mathrm{~d} t \cdot 2\sin x\cos x\).
\(g^{\prime\prime}\left( x \right)=e^{x^{2}}\cdot 2x\sin^{3} x+e^{x^{2}}\cdot 3\sin^{2} x\cos x+2e^{x^{2}}\sin x\cos x+\int_{0}^{x} e^{t^{2}} \mathrm{~d} t \cdot 2\cos 2x\).
\(f^{\prime}\left( 0 \right)=0\),\(f^{\prime\prime}\left( 0 \right)=1>0\),所以 \(x=0\) 是 \(f\left( x \right)\) 的极值点,但不是拐点.
\(g^{\prime}\left( 0 \right)=0\),\(g^{\prime\prime}\left( 0 \right)=0\).
继续求导可得 \(g^{\prime\prime\prime}\left( x \right)=2e^{x^{2}}\sin^{3} x+x\left( 2e^{x^{2}}\sin^{3} x \right)+4\cos 2x , e^{x^{2}}+2\sin 2x\left( e^{x^{2}} \right)-4\sin 2x\int_{0}^{x} e^{t^{2}} \mathrm{~d} t+2\cos 2x , e^{x^{2}}\).
\(g^{\prime\prime\prime}\left( 0 \right)=6>0\),故过 \(x=0\) 为 \(g\left( x \right)\) 的拐点.
3
如果对微分方程 \(y^{\prime\prime}-2ay^{\prime}+\left( a+2 \right)y=0\) 的任一解 \(y\left( x \right)\),反常积分 \(\int_{0}^{+\infty} y\left( x \right) \mathrm{~d} x\) 均收敛,那么 \(a\) 的取值范围是
A. \(\left( -2,-1 \right]\)
B. \(\left( -\infty,-1 \right]\)
C. \(\left( -2,0 \right)\)
D. \(\left( -\infty,0 \right)\)
答案:C
解析:
特征方程为 \(r^{2}-2ar+\left( a+2 \right)=0\).
要使任一解对应的反常积分 \(\int_{0}^{+\infty} y\left( x \right) \mathrm{~d} x\) 均收敛,须有两个特征根都小于 \(0\),即 \(\dfrac{a+2}{1}>0\),\(a<0\),\(\dfrac{-2a}{1}<0\).
故 \(-2<a<0\).
4
设函数 \(f\left( x \right)\),\(g\left( x \right)\) 在 \(x=0\) 的某去心邻域内有定义且恒不为零.若当 \(x\to 0\) 时,\(f\left( x \right)\) 是 \(g\left( x \right)\) 的高阶无穷小,则当 \(x\to 0\) 时,
A. \(f\left( x \right)+g\left( x \right)=o\left( g\left( x \right) \right)\)
B. \(f\left( x \right)g\left( x \right)=o\left( f^{2}\left( x \right) \right)\)
C. \(f\left( x \right)=o\left( e^{g\left( x \right)}-1 \right)\)
D. \(f\left( x \right)=o\left( g^{2}\left( x \right) \right)\)
答案:C
解析:
由题意知 \(f\left( x \right)=o\left( g\left( x \right) \right)\),即 \(\lim\limits_{x\to 0}\dfrac{f\left( x \right)}{g\left( x \right)}=0\).
对于 A,\(\lim\limits_{x\to 0}\dfrac{f\left( x \right)+g\left( x \right)}{g\left( x \right)}=0+1=1\),不是无穷小.
对于 B,\(\lim\limits_{x\to 0}\dfrac{f\left( x \right)g\left( x \right)}{f^{2}\left( x \right)}=\lim\limits_{x\to 0}\dfrac{g\left( x \right)}{f\left( x \right)}=\infty\).
对于 C,\(\lim\limits_{x\to 0}\dfrac{f\left( x \right)}{e^{g\left( x \right)}-1}=\lim\limits_{x\to 0}\dfrac{f\left( x \right)}{g\left( x \right)}=0\).
对于 D,\(\lim\limits_{x\to 0}\dfrac{f\left( x \right)}{g^{2}\left( x \right)}=\lim\limits_{x\to 0}\dfrac{f\left( x \right)}{g\left( x \right)}\cdot \dfrac{1}{g\left( x \right)}\),不是未定式,不能推出结论.
5
设函数 \(f\left( x,y \right)\) 连续,则 \(\int_{-2}^{2} \mathrm{d} x \int_{4-x^{2}}^{2} f\left( x,y \right)\mathrm{d} y=\)
A. \(\int_{0}^{4}\left[ \int_{-2}^{-\sqrt{4-y}} f\left( x,y \right)\mathrm{d} x+\int_{\sqrt{4-y}}^{2} f\left( x,y \right)\mathrm{d} x \right]\mathrm{d} y\)
B. \(\int_{0}^{4}\left[ \int_{-2}^{\sqrt{4-y}} f\left( x,y \right)\mathrm{d} x+\int_{\sqrt{4-y}}^{2} f\left( x,y \right)\mathrm{d} x \right]\mathrm{d} y\)
C. \(\int_{0}^{4}\left[ \int_{-2}^{-\sqrt{4-y}} f\left( x,y \right)\mathrm{d} x+\int_{2}^{\sqrt{4-y}} f\left( x,y \right)\mathrm{d} x \right]\mathrm{d} y\)
D. \(2\int_{0}^{4} \mathrm{d} y \int_{\sqrt{4-y}}^{2} f\left( x,y \right)\mathrm{d} x\)
答案:A
解析:
原式表示的区域为 \(-2\le x\le 2\),\(4-x^{2}\le y\le 2\).交换积分次序后可得
\(\int_{-2}^{2} \mathrm{d} x \int_{4-x^{2}}^{2} f\left( x,y \right)\mathrm{d} y=\int_{0}^{4}\left[ \int_{-2}^{-\sqrt{4-y}} f\left( x,y \right)\mathrm{d} x+\int_{\sqrt{4-y}}^{2} f\left( x,y \right)\mathrm{d} x \right]\mathrm{d} y\).
6
设单位质点 \(P\),\(Q\) 分别位于点 \(\left( 0,0 \right)\) 和 \(\left( 0,1 \right)\) 处,\(P\) 从点 \(\left( 0,0 \right)\) 出发沿 \(x\) 轴正向移动,记 \(G\) 为引力常量,则当质点 \(P\) 移动到点 \(\left( 1,0 \right)\) 时,克服质点 \(Q\) 的引力所做的功为
A. \(\int_{0}^{1}\dfrac{G}{x^{2}+1}\mathrm{d} x\)
B. \(\int_{0}^{1}\dfrac{Gx}{\left( x^{2}+1 \right)^{\frac{3}{2}}}\mathrm{d} x\)
C. \(\int_{0}^{1}\dfrac{G}{\left( x^{2}+1 \right)^{\frac{3}{2}}}\mathrm{d} x\)
D. \(\int_{0}^{1}\dfrac{G\left( x+1 \right)}{\left( x^{2}+1 \right)^{\frac{3}{2}}}\mathrm{d} x\)
答案:B
解析:
当 \(P\) 运动到 \(\left( x,0 \right)\) 时,\(\overrightarrow{QP}=\left( x,-1 \right)\),两点间距离为 \(\sqrt{x^{2}+1}\).
引力沿 \(x\) 方向的分量为 \(\dfrac{Gx}{\left( x^{2}+1 \right)^{\frac{3}{2}}}\),故克服引力所做的功为
\(\int_{0}^{1}\dfrac{Gx}{\left( x^{2}+1 \right)^{\frac{3}{2}}}\mathrm{d} x\).
7
设函数 \(f\left( x \right)\) 连续,给出下列四个条件:
① \(\lim\limits_{x\to 0}\dfrac{\left| f\left( x \right) \right|-f\left( 0 \right)}{x}\) 存在;
② \(\lim\limits_{x\to 0}\dfrac{f\left( x \right)-\left| f\left( 0 \right) \right|}{x}\) 存在;
③ \(\lim\limits_{x\to 0}\dfrac{\left| f\left( x \right) \right|}{x}\) 存在;
④ \(\lim\limits_{x\to 0}\dfrac{\left| f\left( x \right) \right|-\left| f\left( 0 \right) \right|}{x}\) 存在.
其中能得到“\(f\left( x \right)\) 在 \(x=0\) 处可导”的条件的个数是
A. 1
B. 2
C. 3
D. 4
答案:D
解析:
① 若 \(\lim\limits_{x\to 0}\dfrac{\left| f\left( x \right) \right|-f\left( 0 \right)}{x}\) 存在,则分子极限为 \(0\).由连续性得 \(\lim\limits_{x\to 0}\left| f\left( x \right) \right|=\left| f\left( 0 \right) \right|\),故 \(\left| f\left( 0 \right) \right|=f\left( 0 \right)\),从而 \(f\left( 0 \right)\ge 0\).若 \(f\left( 0 \right)>0\),则在 \(0\) 的某邻域内 \(f\left( x \right)>0\),故原极限就是 \(\lim\limits_{x\to 0}\dfrac{f\left( x \right)-f\left( 0 \right)}{x}\).若 \(f\left( 0 \right)=0\),则由左右极限比较可得导数为 \(0\).故 ① 正确.
② 由极限存在及连续性得 \(f\left( 0 \right)=\left| f\left( 0 \right) \right|\ge 0\),再将其化为与 ① 类似情形,可得 \(f\left( x \right)\) 在 \(x=0\) 处可导.故 ② 正确.
③ 设 \(\lim\limits_{x\to 0}\dfrac{\left| f\left( x \right) \right|}{x}=A\),则左右极限存在.比较左右极限可得 \(A=-A=0\),从而 \(\lim\limits_{x\to 0}\dfrac{f\left( x \right)}{x}=0\),故可导.故 ③ 正确.
④ 当 \(f\left( 0 \right)>0\) 时,与 ① 类似;当 \(f\left( 0 \right)=0\) 时,与 ③ 类似;当 \(f\left( 0 \right)<0\) 时,在 \(0\) 的某邻域内 \(f\left( x \right)<0\),原式与 \(\dfrac{-f\left( x \right)+f\left( 0 \right)}{x}\) 只差一个负号,仍可推出可导.故 ④ 正确.
综上,选 D.
8
设矩阵 \(\left( \begin{array}{ccc} 1 & 2 & 0 \ 2 & a & 0 \ 0 & 0 & b \end{array} \right)\) 有一个正特征值和两个负特征值,则
A. \(a>4\),\(b>0\)
B. \(a<4\),\(b>0\)
C. \(a>4\),\(b<0\)
D. \(a<4\),\(b<0\)
答案:D
解析:
由题意,
\(\left| \begin{array}{ccc} 1 & 2 & 0 \\ 2 & a & 0 \\ 0 & 0 & b \end{array} \right|=b\left( a-4 \right)>0\).
故有 \(a>4,b>0\) 或 \(a<4,b<0\).
又
\(\left| \lambda \boldsymbol{E}-\left( \begin{array}{ccc} 1 & 2 & 0 \\ 2 & a & 0 \\ 0 & 0 & b \end{array} \right) \right|=\left( b-\lambda \right)\left[ \lambda^{2}-\left( a-1 \right)\lambda-4 \right]\).
由于 \(\lambda^{2}-\left( a-1 \right)\lambda-4=0\) 有两个异号的根,故第三个特征值必须为负,即 \(b<0\),于是 \(a<4\),\(b<0\).
9
下列矩阵中,可以经过若干初等变换得到矩阵 \(\left( \begin{array}{cccc} 1 & 1 & 0 & 1 \\ 0 & 0 & 1 & 2 \\ 0 & 0 & 0 & 0 \end{array} \right)\) 的是
A. \(\left( \begin{array}{cccc} 1 & 1 & 0 & 1 \\ 1 & 2 & 1 & 3 \\ 2 & 3 & 1 & 4 \end{array} \right)\)
B. \(\left( \begin{array}{cccc} 1 & 1 & 0 & 1 \\ 1 & 1 & 2 & 5 \\ 1 & 1 & 1 & 3 \end{array} \right)\)
C. \(\left( \begin{array}{cccc} 1 & 0 & 0 & 1 \\ 0 & 1 & 0 & 3 \\ 0 & 1 & 0 & 0 \end{array} \right)\)
D. \(\left( \begin{array}{cccc} 1 & 1 & 2 & 3 \\ 1 & 2 & 2 & 3 \\ 2 & 3 & 4 & 6 \end{array} \right)\)
答案:B
解析:
对 B 进行初等行变换:
\(\left( \begin{array}{cccc} 1 & 1 & 0 & 1 \\ 1 & 1 & 2 & 5 \\ 1 & 1 & 1 & 3 \end{array} \right)\to \left( \begin{array}{cccc} 1 & 1 & 0 & 1 \\ 0 & 0 & 1 & 2 \\ 0 & 0 & 0 & 0 \end{array} \right)\).
10
设 3 阶矩阵 \(\boldsymbol{A}\),\(\boldsymbol{B}\) 满足 \(r\left( \boldsymbol{A}\boldsymbol{B} \right)=r\left( \boldsymbol{B}\boldsymbol{A} \right)+1\),则
A. 方程组 \(\left( \boldsymbol{A}+\boldsymbol{B} \right)\boldsymbol{x}=0\) 只有零解.
B. 方程组 \(\boldsymbol{A}\boldsymbol{x}=0\) 与方程组 \(\boldsymbol{B}\boldsymbol{x}=0\) 均只有零解.
C. 方程组 \(\boldsymbol{A}\boldsymbol{x}=0\) 与方程组 \(\boldsymbol{B}\boldsymbol{x}=0\) 没有公共非零解.
D. 方程组 \(\boldsymbol{A}\boldsymbol{B}\boldsymbol{A}\boldsymbol{x}=0\) 与方程组 \(\boldsymbol{B}\boldsymbol{A}\boldsymbol{B}\boldsymbol{x}=0\) 有公共非零解.
答案:D
解析:
取
\(\boldsymbol{A}=\left( \begin{array}{ccc} 1 & 1 & 1 \\ -1 & -1 & -1 \\ 0 & 0 & 0 \end{array} \right)\),\(\boldsymbol{B}=\left( \begin{array}{ccc} 1 & 1 & 1 \\ 1 & 1 & 1 \\ 1 & 1 & 1 \end{array} \right)\).
则
\(\boldsymbol{A}\boldsymbol{B}=\left( \begin{array}{ccc} 3 & 3 & 3 \\ -3 & -3 & -3 \\ 0 & 0 & 0 \end{array} \right)\),\(\boldsymbol{B}\boldsymbol{A}=\left( \begin{array}{ccc} 0 & 0 & 0 \\ 0 & 0 & 0 \\ 0 & 0 & 0 \end{array} \right)\).
故 \(r\left( \boldsymbol{A}\boldsymbol{B} \right)=1=r\left( \boldsymbol{B}\boldsymbol{A} \right)+1\).
由此可知,A 错;\(\boldsymbol{A}\boldsymbol{x}=0\) 与 \(\boldsymbol{B}\boldsymbol{x}=0\) 均有非零解,故 B 错;并且二者有公共非零解,故 C 错;故选 D.
二、填空题
第 11~16 小题,每小题 5 分,共 30 分.
11
设 \(\int_{1}^{+\infty}\dfrac{a}{x\left( 2x+a \right)}\mathrm{d} x=\ln 2\),则 \(a=\) __.
答案:2
解析:
\(\int_{1}^{+\infty}\dfrac{a}{x\left( 2x+a \right)}\mathrm{d} x=2\int_{1}^{+\infty}\left( \dfrac{1}{x}-\dfrac{1}{2x+a} \right)\mathrm{d} x\).
\(=\ln \left| \dfrac{2x}{2x+a} \right| \Big|_{1}^{+\infty}=\ln \left| \dfrac{2+a}{2} \right|=\ln 2\).
所以 \(\left| \dfrac{2+a}{2} \right|=2\).
解得 \(a=2\) 或 \(a=-6\).若 \(a=-6\),则积分在 \(x=3\) 处发散,舍去.故 \(a=2\).
12
曲线 \(y=\sqrt[3]{x^{3}-3x^{2}+1}\) 的渐近线方程为 __.
答案:\(y=x-1\)
解析:
\(\lim\limits_{x\to \infty} y=\infty\),无水平渐近线.
\(\lim\limits_{x\to \infty}\dfrac{y}{x}=1\).
又
\(\lim\limits_{x\to \infty}\left( y-x \right)=\lim\limits_{x\to \infty}\left( \sqrt[3]{x^{3}-3x^{2}+1}-x \right)\)
\(=\lim\limits_{x\to \infty}\dfrac{x^{3}-3x^{2}+1-x^{3}}{\sqrt[3]{\left( x^{3}-3x^{2}+1 \right)^{2}}+x\sqrt[3]{x^{3}-3x^{2}+1}+x^{2}}=-1\).
所以有斜渐近线 \(y=x-1\).
13
\(\lim\limits_{n\to \infty}\dfrac{1}{n^{2}}\left[ \ln \dfrac{1}{n}+2\ln \dfrac{2}{n}+\cdots+\left( n-1 \right)\ln \dfrac{n-1}{n} \right]=\) __.
答案:\(-\dfrac{1}{4}\)
解析:
\(\lim\limits_{n\to \infty}\dfrac{1}{n^{2}}\left[ \ln \dfrac{1}{n}+2\ln \dfrac{2}{n}+\cdots+\left( n-1 \right)\ln \dfrac{n-1}{n} \right]\)
\(=\lim\limits_{n\to \infty}\sum_{k=1}^{n-1}\dfrac{k}{n}\ln \dfrac{k}{n}\cdot \dfrac{1}{n}\)
\(=\int_{0}^{1} x\ln x \mathrm{~d} x=-\dfrac{1}{4}\).
14
已知函数 \(y=y\left( x \right)\) 由
\(x=\ln \left( 1+2t \right)\),
\(2t-\int_{1}^{y+t^{2}} e^{-u^{2}} \mathrm{~d} u=0\)
确定,则 \(y^{\prime}\left( 0 \right)=\) __.
答案:\(e\)
解析:
\(t=0\) 代入方程得 \(y=1\).
对 \(2t-\int_{1}^{y+t^{2}} e^{-u^{2}} \mathrm{~d} u=0\) 关于 \(t\) 求导,得
\(2-e^{-\left( y+t^{2} \right)^{2}}\left( \dfrac{\mathrm{d} y}{\mathrm{d} t}+2t \right)=0\).
代入 \(t=0\),\(y=1\),得 \(\left. \dfrac{\mathrm{d} y}{\mathrm{d} t} \right|_{t=0}=2e\).
又
\(\left. \dfrac{\mathrm{d} x}{\mathrm{d} t} \right|*{t=0}=\left. \dfrac{2}{1+2t} \right|*{t=0}=2\).
所以
\(y^{\prime}\left( 0 \right)=\left. \dfrac{\mathrm{d} y / \mathrm{d} t}{\mathrm{d} x / \mathrm{d} t} \right|_{t=0}=e\).
15
微分方程 \(\left( 2y-3x \right)\mathrm{d} x+\left( 2x-5y \right)\mathrm{d} y=0\) 满足条件 \(y\left( 1 \right)=1\) 的解为 __.
答案:\(5y^{2}-4xy+3x^{2}=4\)
解析:
\(\dfrac{\mathrm{d} y}{\mathrm{d} x}=\dfrac{2y-3x}{5y-2x}=\dfrac{2\dfrac{y}{x}-3}{5\dfrac{y}{x}-2}\).
令 \(\dfrac{y}{x}=u\),则 \(y=ux\),代入得
\(u+x\dfrac{\mathrm{d} u}{\mathrm{d} x}=\dfrac{2u-3}{5u-2}\).
化简为
\(\dfrac{5u-2}{5u^{2}-4u+3}\mathrm{d} u=-\dfrac{1}{x}\mathrm{d} x\).
两边积分得 \(5y^{2}-4xy+3x^{2}=C\).
将 \(y\left( 1 \right)=1\) 代入得 \(C=4\).
故解为 \(5y^{2}-4xy+3x^{2}=4\).
16
设矩阵 \(\boldsymbol{A}=\left( \alpha_{1},\alpha_{2},\alpha_{3},\alpha_{4} \right)\).若 \(\alpha_{1},\alpha_{2},\alpha_{3}\) 线性无关,且 \(\alpha_{1}+\alpha_{2}=\alpha_{3}+\alpha_{4}\),则方程组 \(\boldsymbol{A}\boldsymbol{x}=\alpha_{1}+4\alpha_{4}\) 的通解 \(\boldsymbol{x}=\) __.
答案:\(\boldsymbol{x}=k\left( \begin{array}{c} 1 \ 1 \ -1 \ -1 \end{array} \right)+\left( \begin{array}{c} 1 \ 0 \ 0 \ 4 \end{array} \right)\)
解析:
由 \(\alpha_{1}+\alpha_{2}=\alpha_{3}+\alpha_{4}\),得 \(\alpha_{4}=\alpha_{1}+\alpha_{2}-\alpha_{3}\).
故 \(r\left( \alpha_{1},\alpha_{2},\alpha_{3},\alpha_{4} \right)=r\left( \alpha_{1},\alpha_{2},\alpha_{3} \right)=3=r\left( \boldsymbol{A} \right)\).
所以齐次方程 \(\boldsymbol{A}\boldsymbol{x}=0\) 的基础解系中有 1 个线性无关解向量,
\(\left( 1,1,-1,-1 \right)^{T}\) 为 \(\boldsymbol{A}\boldsymbol{x}=0\) 的解.
而 \(\left( 1,0,0,4 \right)^{T}\) 为 \(\boldsymbol{A}\boldsymbol{x}=\alpha_{1}+4\alpha_{4}\) 的一个解.
故通解为
\(\boldsymbol{x}=k\left( \begin{array}{c} 1 \ 1 \ -1 \ -1 \end{array} \right)+\left( \begin{array}{c} 1 \ 0 \ 0 \ 4 \end{array} \right)\).
三、解答题
第 17~22 小题,共 70 分.解答应写出文字说明、证明过程或演算步骤.
17
本题满分 10 分.
计算 \(\int_{0}^{1}\dfrac{1}{\left( x+1 \right)\left( x^{2}-2x+2 \right)}\mathrm{d} x\).
答案:\(\dfrac{3}{10}\ln 2+\dfrac{\pi}{10}\)
解析:
设
\(\dfrac{1}{\left( 1+x \right)\left( x^{2}-2x+2 \right)}=\dfrac{a}{1+x}+\dfrac{bx+c}{x^{2}-2x+2}\).
则
\(\dfrac{1}{\left( 1+x \right)\left( x^{2}-2x+2 \right)}=\dfrac{\left( a+b \right)x^{2}+\left( -2a+b+c \right)x+2a+c}{\left( 1+x \right)\left( x^{2}-2x+2 \right)}\).
比较系数得
\(\left\{ \begin{array}{l} a+b=0 \\ -2a+b+c=0 \ 2a+c=1 \end{array} \right.\),
解得
\(\left\{ \begin{array}{l} a=\dfrac{1}{5} \\ b=-\dfrac{1}{5} \\ c=\dfrac{3}{5} \end{array} \right.\).
于是
\(\int_{0}^{1}\dfrac{1}{\left( 1+x \right)\left( x^{2}-2x+2 \right)}\mathrm{d} x=\int_{0}^{1}\left[ \dfrac{1}{5\left( 1+x \right)}+\dfrac{-\dfrac{1}{5}x+\dfrac{3}{5}}{x^{2}-2x+2} \right]\mathrm{d} x\).
\(=\dfrac{1}{5}\ln \left( 1+x \right)\Big|*{0}^{1}-\dfrac{1}{5}\int*{0}^{1}\dfrac{x-3}{x^{2}-2x+2}\mathrm{d} x\).
\(=\dfrac{1}{5}\ln 2-\dfrac{1}{5}\left[ \dfrac{1}{2}\int_{0}^{1}\dfrac{1}{x^{2}-2x+2}\mathrm{d}\left( x^{2}-2x+2 \right)-\int_{0}^{1}\dfrac{2}{x^{2}-2x+2}\mathrm{d} x \right]\).
\(=\dfrac{1}{5}\ln 2-\dfrac{1}{10}\ln \left( x^{2}-2x+2 \right)\Big|*{0}^{1}+\dfrac{2}{5}\int*{0}^{1}\dfrac{1}{\left( x-1 \right)^{2}+1}\mathrm{d} x\).
\(=\dfrac{1}{5}\ln 2-\dfrac{1}{10}\left( 0-\ln 2 \right)+\dfrac{2}{5}\arctan \left( x-1 \right)\Big|_{0}^{1}\).
\(=\dfrac{1}{5}\ln 2+\dfrac{1}{10}\ln 2+\dfrac{2}{5}\left( 0+\dfrac{\pi}{4} \right)=\dfrac{3}{10}\ln 2+\dfrac{\pi}{10}\).
18
本题满分 12 分.
设函数 \(f\left( x \right)\) 在 \(x=0\) 处连续,且
\(\lim\limits_{x\to 0}\dfrac{xf\left( x \right)-e^{2\sin x}+1}{\ln \left( 1+x \right)+\ln \left( 1-x \right)}=-3\),
证明 \(f\left( x \right)\) 在 \(x=0\) 处可导,并求 \(f^{\prime}\left( 0 \right)\).
答案:\(f^{\prime}\left( 0 \right)=5\)
解析:
由题设,
\(-3=\lim\limits_{x\to 0}\dfrac{xf\left( x \right)-e^{2\sin x}+1}{\ln \left( 1+x \right)+\ln \left( 1-x \right)}\)
\(=\lim\limits_{x\to 0}\dfrac{xf\left( x \right)-e^{2\sin x}+1}{\ln \left( 1-x^{2} \right)}\)
\(=\lim\limits_{x\to 0}\dfrac{xf\left( x \right)-e^{2\sin x}+1}{-x^{2}}\).①
又
\(=\lim\limits_{x\to 0}\dfrac{f\left( x \right)+\dfrac{1-e^{2\sin x}}{x}}{-x}\).
因为
\(\lim\limits_{x\to 0}\dfrac{1-e^{2\sin x}}{x}=-2\).
由 ① 知
\(-3=\lim\limits_{x\to 0}\dfrac{x\left[ f\left( x \right)-f\left( 0 \right) \right]+2x-e^{2\sin x}+1}{-x^{2}}\)
\(=-\lim\limits_{x\to 0}\dfrac{f\left( x \right)-f\left( 0 \right)}{x}+\lim\limits_{x\to 0}\dfrac{2x-e^{2\sin x}+1}{-x^{2}}\)
\(=-\lim\limits_{x\to 0}\dfrac{f\left( x \right)-f\left( 0 \right)}{x}+\lim\limits_{x\to 0}\dfrac{2-2\cos x , e^{2\sin x}}{-2x}\)
\(=-\lim\limits_{x\to 0}\dfrac{f\left( x \right)-f\left( 0 \right)}{x}+\lim\limits_{x\to 0}\dfrac{1-\cos x+\cos x\left( 1-e^{2\sin x} \right)}{-x}\)
\(=-\lim\limits_{x\to 0}\dfrac{f\left( x \right)-f\left( 0 \right)}{x}+2\).
所以
\(\lim\limits_{x\to 0}\dfrac{f\left( x \right)-f\left( 0 \right)}{x}=5\),
即 \(f\left( x \right)\) 在 \(x=0\) 处可导,且 \(f^{\prime}\left( 0 \right)=5\).
19
本题满分 12 分.
设函数 \(f\left( x,y \right)\) 可微且满足 \(\mathrm{d} f\left( x,y \right)=-2xe^{-y}\mathrm{d} x+e^{-y}\left( x^{2}-y-1 \right)\mathrm{d} y\),\(f\left( 0,0 \right)=2\),求 \(f\left( x,y \right)\),并求 \(f\left( x,y \right)\) 的极值.
答案:\(f\left( x,y \right)=-x^{2}e^{-y}+\left( y+2 \right)e^{-y}\);\(f\left( 0,-1 \right)\) 为极大值点.
解析:
由题意知
\(f_{x}^{\prime}\left( x,y \right)=-2xe^{-y}\),\(f_{y}^{\prime}\left( x,y \right)=e^{-y}\left( x^{2}-y-1 \right)\).
故
\(f\left( x,y \right)=\int -2xe^{-y}\mathrm{d} x=-x^{2}e^{-y}+C\left( y \right)\).
于是
\(f_{y}^{\prime}\left( x,y \right)=x^{2}e^{-y}+C^{\prime}\left( y \right)=e^{-y}\left( x^{2}-y-1 \right)\).
所以
\(C^{\prime}\left( y \right)=-\left( y+1 \right)e^{-y}\),
从而
\(C\left( y \right)=\left( y+2 \right)e^{-y}+C\).
故
\(f\left( x,y \right)=-x^{2}e^{-y}+\left( y+2 \right)e^{-y}+C\).
由 \(f\left( 0,0 \right)=2\),得 \(C=0\).
因此
\(f\left( x,y \right)=-x^{2}e^{-y}+\left( y+2 \right)e^{-y}\).
令
\(\left\{ \begin{array}{l} f_{x}^{\prime}\left( x,y \right)=-2xe^{-y}=0 \\ f_{y}^{\prime}\left( x,y \right)=e^{-y}\left( x^{2}-y-1 \right)=0 \end{array} \right.\),
解得
\(\left\{ \begin{array}{l} x=0 \\ y=-1 \end{array} \right.\).
再求二阶偏导数:
\(f_{xx}^{\prime\prime}\left( x,y \right)=-2e^{-y}\),
\(f_{xy}^{\prime\prime}\left( x,y \right)=2xe^{-y}\),
\(f_{yy}^{\prime\prime}\left( x,y \right)=-e^{-y}\left( x^{2}-y-1 \right)-e^{-y}\).
在 \(\left( 0,-1 \right)\) 处,
\(A=-2e\),\(B=0\),\(C=-e\),
故
\(AC-B^{2}>0\),且 \(A<0\).
所以 \(\left( 0,-1 \right)\) 为极大值点,极大值为
\(f\left( 0,-1 \right)=e\).
20
本题满分 12 分.
已知平面有界区域 \(D=\left\{ \left( x,y \right)\mid x^{2}+y^{2}\le 4x,\\ x^{2}+y^{2}\le 4y \right\}\),计算二重积分 \(\iint_{D}\left( x-y \right)^{2}\mathrm{d} x \mathrm{d} y\).
答案:\(12\pi-\dfrac{112}{3}\)
解析:
由对称性,
\(\iint_{D}\left( x-y \right)^{2}\mathrm{d} x \mathrm{d} y=2\iint_{D_{1}}\left( x^{2}+y^{2}-2xy \right)\mathrm{d} x \mathrm{d} y\).
化为极坐标,取
\(x=r\cos \theta\),\(y=r\sin \theta\),
则
\(=2\int_{0}^{\frac{\pi}{4}} \mathrm{d} \theta \int_{0}^{4\sin \theta}\left( r^{2}-2r^{2}\cos \theta \sin \theta \right)r\mathrm{d} r\).
\(=128\int_{0}^{\frac{\pi}{4}}\left( \sin^{4}\theta-2\cos \theta \sin^{5}\theta \right)\mathrm{d} \theta\)
\(=128\left[ \int_{0}^{\frac{\pi}{4}}\left( \dfrac{1-\cos 2\theta}{2} \right)^{2}\mathrm{d} \theta-\dfrac{1}{3}\sin^{6}\theta \Big|_{0}^{\frac{\pi}{4}} \right]\)
\(=128\left[ \dfrac{1}{4}\int_{0}^{\frac{\pi}{4}}\left( 1-2\cos 2\theta+\cos^{2}2\theta \right)\mathrm{d} \theta-\dfrac{1}{24} \right]\)
\(=128\left[ \dfrac{1}{4}\left( \dfrac{\pi}{4}-\sin 2\theta \right)\Big|*{0}^{\frac{\pi}{4}}+\dfrac{1}{2}\int*{0}^{\frac{\pi}{2}}\cos^{2} t \mathrm{d} t-\dfrac{1}{24} \right]\)
\(=128\left( \dfrac{3\pi}{32}-\dfrac{7}{24} \right)=12\pi-\dfrac{112}{3}\).
21
本题满分 12 分.
设函数 \(f\left( x \right)\) 其在区间 \(\left( a,b \right)\) 内可导.证明:导函数 \(f^{\prime}\left( x \right)\) 在 \(\left( a,b \right)\) 内严格单调增加的充分必要条件是:
对 \(\left( a,b \right)\) 内任意的 \(x_{1},x_{2},x_{3}\),当 \(x_{1}<x_{2}<x_{3}\) 时,有
\(\dfrac{f\left( x_{2} \right)-f\left( x_{1} \right)}{x_{2}-x_{1}}<\dfrac{f\left( x_{3} \right)-f\left( x_{2} \right)}{x_{3}-x_{2}}\).
答案:略
解析:
证明:
(1)必要性
由拉格朗日中值定理,
\(\dfrac{f\left( x_{2} \right)-f\left( x_{1} \right)}{x_{2}-x_{1}}=f^{\prime}\left( \xi_{1} \right)\),其中 \(x_{1}<\xi_{1}<x_{2}\);
\(\dfrac{f\left( x_{3} \right)-f\left( x_{2} \right)}{x_{3}-x_{2}}=f^{\prime}\left( \xi_{2} \right)\),其中 \(x_{2}<\xi_{2}<x_{3}\).
由于 \(f^{\prime}\left( x \right)\) 在 \(\left( a,b \right)\) 上单增,且 \(\xi_{1}<\xi_{2}\),故
\(f^{\prime}\left( \xi_{1} \right)<f^{\prime}\left( \xi_{2} \right)\),
即
\(\dfrac{f\left( x_{2} \right)-f\left( x_{1} \right)}{x_{2}-x_{1}}<\dfrac{f\left( x_{3} \right)-f\left( x_{2} \right)}{x_{3}-x_{2}}\).
(2)充分性
对任意 \(c_{1}<c_{2}\in \left( a,b \right)\),有
\(f^{\prime}\left( c_{1} \right)=\lim\limits_{x\to c_{1}}\dfrac{f\left( x \right)-f\left( c_{1} \right)}{x-c_{1}}\),
\(f^{\prime}\left( c_{2} \right)=\lim\limits_{x\to c_{2}}\dfrac{f\left( x \right)-f\left( c_{2} \right)}{x-c_{2}}\).
当 \(a<c_{1}<x<c_{2}<b\) 时,由已知条件可知
\(\dfrac{f\left( c_{1} \right)-f\left( a \right)}{c_{1}-a}<\dfrac{f\left( x \right)-f\left( c_{1} \right)}{x-c_{1}}<\dfrac{f\left( c_{2} \right)-f\left( x \right)}{c_{2}-x}\).
两边同时取极限,并利用极限保号性,可得
\(\lim\limits_{x\to c_{1}^{+}}\dfrac{f\left( x \right)-f\left( c_{1} \right)}{x-c_{1}}\le \lim\limits_{x\to c_{1}^{+}}\dfrac{f\left( c_{2} \right)-f\left( x \right)}{c_{2}-x}=\dfrac{f\left( c_{2} \right)-f\left( c_{1} \right)}{c_{2}-c_{1}}\),
\(\lim\limits_{x\to c_{2}^{-}}\dfrac{f\left( c_{2} \right)-f\left( x \right)}{c_{2}-x}\ge \lim\limits_{x\to c_{2}^{-}}\dfrac{f\left( x \right)-f\left( c_{1} \right)}{x-c_{1}}=\dfrac{f\left( c_{2} \right)-f\left( c_{1} \right)}{c_{2}-c_{1}}\).
从而
\(f^{\prime}\left( c_{1} \right)=\lim\limits_{x\to c_{1}^{+}}\dfrac{f\left( x \right)-f\left( c_{1} \right)}{x-c_{1}}\le \lim\limits_{x\to c_{2}^{-}}\dfrac{f\left( x \right)-f\left( c_{2} \right)}{x-c_{2}}=f^{\prime}\left( c_{2} \right)\).
故 \(f^{\prime}\left( x \right)\) 在 \(\left( a,b \right)\) 上单增.
22
本题满分 12 分.
已知矩阵
\(\boldsymbol{A}=\left( \begin{array}{ccc} 4 & 1 & -2 \\ 1 & 1 & 1 \\ -2 & 1 & a \end{array} \right)\),
\(\boldsymbol{B}=\left( \begin{array}{ccc} k & 0 & 0 \\ 0 & 6 & 0 \\ 0 & 0 & 0 \end{array} \right)\).
(1)求 \(a\) 的值及 \(k\) 的取值范围;
(2)若存在正交矩阵 \(\boldsymbol{Q}\) 使得 \(\boldsymbol{Q}^{T}\boldsymbol{A}\boldsymbol{Q}=\boldsymbol{B}\),求 \(k\) 及 \(\boldsymbol{Q}\).
答案:
(1)\(a=4\),\(k>0\);
(2)\(k=3\),\(\boldsymbol{Q}=\left( \begin{array}{ccc} \dfrac{1}{\sqrt{3}} & -\dfrac{1}{\sqrt{2}} & \dfrac{1}{\sqrt{6}} \ \dfrac{1}{\sqrt{3}} & 0 & -\dfrac{2}{\sqrt{6}} \ \dfrac{1}{\sqrt{3}} & \dfrac{1}{\sqrt{2}} & \dfrac{1}{\sqrt{6}} \end{array} \right)\).
解析:
(1)因为 \(\boldsymbol{A}\) 与 \(\boldsymbol{B}\) 合同,所以 \(\lambda=0\) 为 \(\boldsymbol{A}\) 的一个特征值.
于是 \(\left| \boldsymbol{A} \right|=0\),得 \(a=4\).
再由 \(\left| \lambda \boldsymbol{E}-\boldsymbol{A} \right|=0\),得 \(\lambda_{1}=3\),\(\lambda_{2}=6\),\(\lambda_{3}=0\),故 \(k>0\).
(2)因为存在正交矩阵 \(\boldsymbol{Q}\),使得 \(\boldsymbol{Q}^{T}\boldsymbol{A}\boldsymbol{Q}=\boldsymbol{B}\),所以 \(k=3\).
当 \(\lambda_{1}=3\) 时,由 \(\left( 3\boldsymbol{E}-\boldsymbol{A} \right)\boldsymbol{x}=0\),可取特征向量
\(\boldsymbol{\xi}_{1}=\left( \begin{array}{c} 1 \ 1 \ 1 \end{array} \right)\).
当 \(\lambda_{2}=6\) 时,由 \(\left( 6\boldsymbol{E}-\boldsymbol{A} \right)\boldsymbol{x}=0\),可取特征向量
\(\boldsymbol{\xi}_{2}=\left( \begin{array}{c} -1 \ 0 \ 1 \end{array} \right)\).
当 \(\lambda_{3}=0\) 时,由 \(\left( 0\boldsymbol{E}-\boldsymbol{A} \right)\boldsymbol{x}=0\),可取特征向量
\(\boldsymbol{\xi}_{3}=\left( \begin{array}{c} 1 \ -2 \ 1 \end{array} \right)\).
将 \(\boldsymbol{\xi}*{1}\),\(\boldsymbol{\xi}*{2}\),\(\boldsymbol{\xi}_{3}\) 单位化,得
\(\boldsymbol{Q}=\left( \begin{array}{ccc} \dfrac{1}{\sqrt{3}} & -\dfrac{1}{\sqrt{2}} & \dfrac{1}{\sqrt{6}} \ \dfrac{1}{\sqrt{3}} & 0 & -\dfrac{2}{\sqrt{6}} \ \dfrac{1}{\sqrt{3}} & \dfrac{1}{\sqrt{2}} & \dfrac{1}{\sqrt{6}} \end{array} \right)\).