2023 National Graduate Entrance Examination Mathematics I Past Paper

Part I: Multiple Choice

Part I: Multiple Choice: Questions 1-10, 5 points each, 50 points in total. Of the four options given in each of the following questions, only one satisfies the requirement of the question.

1. The equation of the asymptote of the curve y=xln⁡(e+1x−1)y=x\ln(e+\frac{1}{x-1}) is ( )

(A) y=x+ey=x+e

(B) y=x+1ey=x+\frac{1}{e}

(C) y=xy=x

(D) y=x−1ey=x-\frac{1}{e}

asymptotelimit calculationlogarithmic function

Approach:

This question tests the method of finding the asymptotes of a curve. The coefficients of the oblique asymptote y=kx+by=kx+b are determined by two limits: kk is the limit of y/xy/x and bb is the limit of y−kxy-kx.

Steps:

  1. The slope: k=lim⁡x→∞yx=lim⁡x→∞xln⁡(e+1x−1)x=lim⁡x→∞ln⁡(e+1x−1)=e0=1k=\lim\limits_{x\to\infty}\dfrac{y}{x}=\lim\limits_{x\to\infty}\dfrac{x\ln\left(e+\dfrac{1}{x-1}\right)}{x}=\lim\limits_{x\to\infty}\ln\left(e+\dfrac{1}{x-1}\right)=e^0=1.
  2. The intercept: b=lim⁡x→∞(y−kx)=lim⁡x→∞[xln⁡(e+1x−1)−x]=lim⁡x→∞x[ln⁡(e+1x−1)−1]b=\lim\limits_{x\to\infty}(y-kx)=\lim\limits_{x\to\infty}\left[x\ln\left(e+\dfrac{1}{x-1}\right)-x\right]=\lim\limits_{x\to\infty}x\left[\ln\left(e+\dfrac{1}{x-1}\right)-1\right].
  3. Using ln⁡(1+u)∼u\ln(1+u)\sim u (u→0u\to0) we get ln⁡(e+1x−1)−1=ln⁡(1+1e(x−1))∼1e(x−1)\ln\left(e+\dfrac{1}{x-1}\right)-1=\ln\left(1+\dfrac{1}{e(x-1)}\right)\sim\dfrac{1}{e(x-1)}, hence b=lim⁡x→∞xe(x−1)=1eb=\lim\limits_{x\to\infty}\dfrac{x}{e(x-1)}=\dfrac1e.
  4. Hence the equation of the oblique asymptote is y=x+1ey=x+\dfrac{1}{e}, so (B) is the correct choice.

Answer:

The equation of the oblique asymptote is y=x+1ey=x+\dfrac{1}{e}, so (B) is the correct choice.

2. If the solutions of the differential equation y′′+ay′+by=0y''+ay'+by=0 are bounded on (−∞,+∞)(-\infty,+\infty), then ( )

(A) a<0,b>0a<0,b>0

(B) a>0,b>0a>0,b>0

(C) a=0,b>0a=0,b>0

(D) a=0,b<0a=0,b<0

differential equationcharacteristic equationboundedness

Approach:

This question tests the relation between the boundedness of the solutions of a second-order linear differential equation with constant coefficients and the characteristic roots. That the solutions are bounded on (−∞,+∞)(-\infty,+\infty) is equivalent to all the roots of the characteristic equation being purely imaginary (with zero real part).

Steps:

  1. The characteristic equation is λ2+aλ+b=0\lambda^2+a\lambda+b=0; denote its discriminant by Δ=a2−4b\Delta=a^2-4b.
  2. When Δ>0\Delta>0 there are two distinct real roots λ1,λ2\lambda_1,\lambda_2, and the general solution is y=C1eλ1x+C2eλ2xy=C_1e^{\lambda_1x}+C_2e^{\lambda_2x}; as soon as one of the roots is nonzero, taking C1,C2C_1,C_2 not both zero makes the solution unbounded.
  3. When Δ=0\Delta=0 there is a repeated root λ=−a2\lambda=-\dfrac a2, and the general solution is y=(C1+C2x)e−a2xy=(C_1+C_2x)e^{-\frac a2x}; if C2≠0C_2\ne0 the solution is unbounded as x→+∞x\to+\infty.
  4. When Δ<0\Delta<0 there is a pair of conjugate complex roots λ1,2=−a2±4b−a22i\lambda_{1,2}=-\dfrac a2\pm\dfrac{\sqrt{4b-a^2}}{2}i, and the general solution is y=e−a2x(C1cos⁡4b−a22x+C2sin⁡4b−a22x)y=e^{-\frac a2x}\left(C_1\cos\dfrac{\sqrt{4b-a^2}}{2}x+C_2\sin\dfrac{\sqrt{4b-a^2}}{2}x\right).
  5. For the solutions to be bounded on the whole real axis, the factor e−a2xe^{-\frac a2x} must be identically 1, that is a=0a=0; then Δ=a2−4b<0\Delta=a^2-4b<0 gives b>0b>0, so (C) is the correct choice.

Answer:

a=0, b>0a=0,\ b>0, so (C) is the correct choice.

3. Let the function y=f(x)y=f(x) be determined by {x=2t+∣t∣y=∣t∣sin⁡t\begin{cases}x=2t+|t|\\y=|t|\sin t\end{cases}, then ( )

(A) f(x)f(x) is continuous and f′(0)f'(0) does not exist

(B) f′(0)f'(0) exists and f′(x)f'(x) is not continuous at x=0x=0

(C) f′(x)f'(x) is continuous and f′′(0)f''(0) does not exist

(D) f′(0)f'(0) exists and f′′(x)f''(x) is not continuous at x=0x=0

parametric equationderivativecontinuity

Approach:

This question tests the differentiability at the breakpoint and the continuity of the derivative of a function determined by parametric equations. First the function is written as a piecewise expression according to the sign of the parameter, and then the left and right derivatives and the second derivative are computed separately.

Steps:

  1. When t≥0t\ge0 we have x=2t+∣t∣=3t, y=tsin⁡tx=2t+|t|=3t,\ y=t\sin t, hence y=x3sin⁡x3y=\dfrac{x}{3}\sin\dfrac{x}{3}; when t<0t<0 we have x=t, y=−tsin⁡tx=t,\ y=-t\sin t, hence y=−xsin⁡xy=-x\sin x.
  2. Thus y={x3sin⁡x3,x≥0,−xsin⁡x,x<0.y=\begin{cases}\dfrac{x}{3}\sin\dfrac{x}{3}, & x\ge0,\\-x\sin x, & x<0.\end{cases}
  3. Computing f′(0)f'(0): f′(0)=lim⁡x→0+sin⁡x33=0f'(0)=\lim\limits_{x\to0^+}\dfrac{\sin\frac x3}{3}=0, f′(0)=lim⁡x→0−(−sin⁡x)=0f'(0)=\lim\limits_{x\to0^-}(-\sin x)=0. The two sides are equal, so f′(0)f'(0) exists and equals 0.
  4. Differentiating once more gives y′(x)={13sin⁡x3+x9cos⁡x3,x≥0,−sin⁡x−xcos⁡x,x<0.y'(x)=\begin{cases}\dfrac13\sin\dfrac x3+\dfrac x9\cos\dfrac x3, & x\ge0,\\-\sin x-x\cos x, & x<0.\end{cases}
  5. Since the right-hand limit lim⁡x→0+13cos⁡x3=13\lim\limits_{x\to0^+}\dfrac13\cos\dfrac x3=\dfrac13 and the left-hand limit lim⁡x→0−(−sin⁡x−xcos⁡x)=0\lim\limits_{x\to0^-}(-\sin x-x\cos x)=0 are not equal, y′′(0)y''(0) does not exist, that is f′′(x)f''(x) is not continuous at x=0x=0, so (D) is the correct choice.

Answer:

f′(0)f'(0) exists (f′(0)=0f'(0)=0), and f′′(x)f''(x) is not continuous at x=0x=0, so (D) is the correct choice.

4. Given an<bn(n=1,2,⋯ )a_n<b_n(n=1,2,\cdots), if the series ∑n=1∞an\sum\limits_{n=1}^{\infty} a_n and ∑n=1∞bn\sum\limits_{n=1}^{\infty} b_n both converge, then the condition that ”∑n=1∞an\sum\limits_{n=1}^{\infty} a_n converges absolutely” is ( )

(A) a sufficient and necessary condition

(B) a sufficient but not necessary condition

(C) a necessary but not sufficient condition

(D) neither a sufficient nor a necessary condition

convergence of a seriesabsolute convergencecomparison test

Approach:

This question tests the comparison test for absolutely convergent series. Since an<bna_n<b_n, the difference series ∑(bn−an)\sum(b_n-a_n) is a convergent series of positive terms, so the absolute convergence of the two series can be converted into each other.

Steps:

  1. From an<bna_n<b_n we have bn−an>0b_n-a_n>0 and ∑n=1∞(bn−an)=∑bn−∑an\sum\limits_{n=1}^{\infty}(b_n-a_n)=\sum b_n-\sum a_n converges, so this series of positive terms converges absolutely.
  2. If ∑an\sum a_n converges absolutely, then from ∣bn∣=∣bn−an+an∣≤∣bn−an∣+∣an∣|b_n|=|b_n-a_n+a_n|\le|b_n-a_n|+|a_n| and the comparison test, ∑bn\sum b_n converges absolutely.
  3. If ∑bn\sum b_n converges absolutely, then from ∣an∣=∣an−bn+bn∣≤∣an−bn∣+∣bn∣|a_n|=|a_n-b_n+b_n|\le|a_n-b_n|+|b_n| and the comparison test, ∑an\sum a_n converges absolutely.
  4. The two implications go both ways, which shows that ”∑an\sum a_n converges absolutely” is neither a sufficient condition nor a necessary condition for ∑an,∑bn\sum a_n,\sum b_n both to converge, so (D) is the correct choice.

Answer:

Neither a sufficient nor a necessary condition, so (D) is the correct choice.

5. Let nn be the order of the matrices A,B,CA,B,C, which satisfy ABC=0ABC=0, and let EE be the identity matrix of order nn. Denote the ranks of the matrices (0ABCE)\begin{pmatrix}0 & A \\ BC & E\end{pmatrix}, (EAB0E)\begin{pmatrix}E & AB \\ 0 & E\end{pmatrix}, (EABAB0)\begin{pmatrix}E & AB \\ AB & 0\end{pmatrix} by γ1,γ2,γ3\gamma_1,\gamma_2,\gamma_3 respectively. Then ( )

(A) γ1≤γ2≤γ3\gamma_1\leq\gamma_2\leq\gamma_3

(B) γ1≤γ3≤γ2\gamma_1\leq\gamma_3\leq\gamma_2

(C) γ3≤γ1≤γ2\gamma_3\leq\gamma_1\leq\gamma_2

(D) γ2≤γ1≤γ3\gamma_2\leq\gamma_1\leq\gamma_3

matrix rankelementary transformationmatrix operation

Approach:

This question tests the rank of block matrices and elementary transformations. Elementary transformations do not change the rank of a matrix, and the three block matrices can be reduced to block diagonal form, which reduces the problem to comparing r(AB)r(AB) with r(ABAB)r(ABAB).

Steps:

  1. Apply an elementary transformation to (0ABCE)\begin{pmatrix}0&A\\BC&E\end{pmatrix}: add AA times the second row to the first row, obtaining (−ABC0BCE)\begin{pmatrix}-ABC&0\\BC&E\end{pmatrix}; since ABC=0ABC=0 this becomes (00BCE)\begin{pmatrix}0&0\\BC&E\end{pmatrix}, whose rank is nn, that is γ1=n\gamma_1=n.
  2. An elementary transformation of (ABC0E)\begin{pmatrix}AB&C\\0&E\end{pmatrix} gives (AB00E)\begin{pmatrix}AB&0\\0&E\end{pmatrix}, so γ2=r(AB)+n\gamma_2=r(AB)+n.
  3. An elementary transformation of (EABAB0)\begin{pmatrix}E&AB\\AB&0\end{pmatrix} gives (E00−ABAB)\begin{pmatrix}E&0\\0&-ABAB\end{pmatrix}, so γ3=n+r(ABAB)\gamma_3=n+r(ABAB).
  4. Since r(ABAB)≤r(AB)r(ABAB)\le r(AB), we get γ1≤γ3≤γ2\gamma_1\le\gamma_3\le\gamma_2, so (B) is the correct choice.

Answer:

γ1≤γ3≤γ2\gamma_1\leq\gamma_3\leq\gamma_2, so (B) is the correct choice.

6. Which of the following matrices cannot be similar to a diagonal matrix ( )

(A) (11a020003)\begin{pmatrix}1 & 1 & a \\ 0 & 2 & 0 \\ 0 & 0 & 3\end{pmatrix}

(B) (11a120a03)\begin{pmatrix}1 & 1 & a \\ 1 & 2 & 0 \\ a & 0 & 3\end{pmatrix}

(C) (11a020002)\begin{pmatrix}1 & 1 & a \\ 0 & 2 & 0 \\ 0 & 0 & 2\end{pmatrix}

(D) (11a022002)\begin{pmatrix}1 & 1 & a \\ 0 & 2 & 2 \\ 0 & 0 & 2\end{pmatrix}

matrix diagonalizationeigenvaluereal symmetric matrix

Approach:

This question tests the necessary and sufficient condition for a matrix to be similar to a diagonal matrix. A matrix is diagonalizable if and only if the geometric multiplicity and the algebraic multiplicity of every eigenvalue are equal, that is, the defect of r(A−λE)r(A-\lambda E) equals the multiplicity.

Steps:

  1. The matrix in option (A) is upper triangular, with the three distinct eigenvalues 1,2,31,2,3, so it is certainly similar to a diagonal matrix.
  2. The matrix in option (B) is a real symmetric matrix, and a real symmetric matrix is always similar to a diagonal matrix, so it too is diagonalizable.
  3. The matrix in option (C) has the eigenvalues 1,2,21,2,2, and for λ=2\lambda=2 we have r(C−2E)=1r(C-2E)=1, so the multiplicity of the double eigenvalue is 2=3−r(C−2E)2=3-r(C-2E); it is diagonalizable.
  4. The matrix in option (D) also has the eigenvalues 1,2,21,2,2, but r(D−2E)≠1r(D-2E)\ne1, that is the multiplicity of the double eigenvalue is 2≠3−r(D−2E)2\ne3-r(D-2E), so it cannot be similar to a diagonal matrix, and (D) is the correct choice.

Answer:

Option (D) cannot be similar to a diagonal matrix, so (D) is the correct choice.

7. Given the vectors α1=(123), α2=(211), β1=(259), β2=(101)\alpha_1=\begin{pmatrix}1\\2\\3\end{pmatrix},\ \alpha_2=\begin{pmatrix}2\\1\\1\end{pmatrix},\ \beta_1=\begin{pmatrix}2\\5\\9\end{pmatrix},\ \beta_2=\begin{pmatrix}1\\0\\1\end{pmatrix}, if γ\gamma can be represented as a linear combination of α1,α2\alpha_1,\alpha_2 and also as a linear combination of β1,β2\beta_1,\beta_2, then γ=\gamma=( )

(A) k(334),k∈Rk\begin{pmatrix}3\\3\\4\end{pmatrix},k\in\mathbb{R}

(B) k(3510),k∈Rk\begin{pmatrix}3\\5\\10\end{pmatrix},k\in\mathbb{R}

(C) k(−112),k∈Rk\begin{pmatrix}-1\\1\\2\end{pmatrix},k\in\mathbb{R}

(D) k(158),k∈Rk\begin{pmatrix}1\\5\\8\end{pmatrix},k\in\mathbb{R}

linear representation of vectorssystem of linear equationsmatrix rank

Approach:

This question tests the linear representation of a vector group and the elementary row transformation of a matrix. Let the same vector be represented linearly by the α\alpha group and by the β\beta group; after the coefficients are combined one obtains a homogeneous system of linear equations, whose fundamental system of solutions is found by elementary row transformation.

Steps:

  1. Put r=x1α1+x2α2=y1β1+y2β2r=x_1\alpha_1+x_2\alpha_2=y_1\beta_1+y_2\beta_2, and after transposing the terms, x1α1+x2α2−y1β1−y2β2=0x_1\alpha_1+x_2\alpha_2-y_1\beta_1-y_2\beta_2=0.
  2. Writing this in matrix form and applying elementary row transformations: (12−2−121−5031−9−1)→(1003010−10011)\begin{pmatrix}1&2&-2&-1\\2&1&-5&0\\3&1&-9&-1\end{pmatrix}\to\begin{pmatrix}1&0&0&3\\0&1&0&-1\\0&0&1&1\end{pmatrix}.
  3. Hence the fundamental system of solutions is (−3,1,−1,1)T(-3,1,-1,1)^T, that is (x1,x2,y1,y2)T=c(−3,1,−1,1)T, c∈R(x_1,x_2,y_1,y_2)^T=c(-3,1,-1,1)^T,\ c\in\mathbb{R}.
  4. Then r=−cβ1+cβ2=−c(2,5,9)T+c(1,0,1)T=(−c,−5c,−8c)T=−c(1,5,8)Tr=-c\beta_1+c\beta_2=-c(2,5,9)^T+c(1,0,1)^T=(-c,-5c,-8c)^T=-c(1,5,8)^T.
  5. Put k=−ck=-c; then r=k(1,5,8)T, k∈Rr=k(1,5,8)^T,\ k\in\mathbb{R}, so (D) is the correct choice.

Answer:

r=k(158), k∈Rr=k\begin{pmatrix}1\\5\\8\end{pmatrix},\ k\in\mathbb{R}, so (D) is the correct choice.

8. Let the random variable XX follow a Poisson distribution with parameter 11. Then E(∣X−EX∣)=E(|X-EX|)=( )

(A) 1e\frac{1}{e}

(B) 12\frac{1}{2}

(C) 2e\frac{2}{e}

(D) 11

Poisson distributionexpectationprobability calculation

Approach:

This question tests the computation of the expectation and the absolute expectation of a Poisson distribution. Write ∣X−EX∣|X-EX| piecewise according to whether XX is zero, and then sum with the probability formula of the Poisson distribution.

Steps:

  1. A Poisson distribution with parameter 1 satisfies EX=1EX=1.
  2. Thus ∣X−EX∣={1,X=0,X−1,X=1,2,⋯ .|X-EX|=\begin{cases}1, & X=0,\\X-1, & X=1,2,\cdots.\end{cases}
  3. Hence E(∣X−EX∣)=1⋅P{X=0}+∑k=1∞(k−1)P{X=k}E(|X-EX|)=1\cdot P\{X=0\}+\sum\limits_{k=1}^{\infty}(k-1)P\{X=k\}.
  4. From P{X=k}=e−1k!P\{X=k\}=\dfrac{e^{-1}}{k!} we get E(∣X−EX∣)=e−1∑kk−1k!+e−1=e−1E(X−1)+e−1=2eE(|X-EX|)=e^{-1}\sum\limits_{k}\dfrac{k-1}{k!}+e^{-1}=e^{-1}E(X-1)+e^{-1}=\dfrac{2}{e}.
  5. Hence (C) is the correct choice.

Answer:

E(∣X−EX∣)=2eE(|X-EX|)=\dfrac{2}{e}, so (C) is the correct choice.

9. Let X1,X2,⋯ ,XnX_1,X_2,\cdots,X_n be a simple random sample from the population N(μ,σ2)N(\mu,\sigma^2), and let Y1,Y2,⋯ ,YmY_1,Y_2,\cdots,Y_m be a simple random sample from the population N(μ2,2σ2)N(\mu_2,2\sigma^2), the two samples being mutually independent. Denote X‾=1n∑i=1nXi\overline{X}=\frac{1}{n}\sum\limits_{i=1}^n X_i, Y‾=1m∑i=1mYi\overline{Y}=\frac{1}{m}\sum\limits_{i=1}^m Y_i, S12=1n−1∑i=1n(Xi−X‾)2S_1^2=\frac{1}{n-1}\sum\limits_{i=1}^n (X_i-\overline{X})^2, S22=1m−1∑i=1m(Yi−Y‾)2S_2^2=\frac{1}{m-1}\sum\limits_{i=1}^m (Y_i-\overline{Y})^2. Then ( )

(A) S12S22∼F(n,m)\frac{S_1^2}{S_2^2}\sim F(n,m)

(B) S12S22∼F(n−1,m−1)\frac{S_1^2}{S_2^2}\sim F(n-1,m-1)

(C) 2S12S22∼F(n,m)\frac{2S_1^2}{S_2^2}\sim F(n,m)

(D) 2S12S22∼F(n−1,m−1)\frac{2S_1^2}{S_2^2}\sim F(n-1,m-1)

F distributionsample variancenormal distribution

Approach:

This question tests the distribution of the ratio of the sample variances of two independent normal samples. The key is to standardize the two sample variances into χ2\chi^2 variables and then use the definition of the FF distribution to obtain the distribution of the ratio.

Steps:

  1. S12=1n−1∑i=1n(Xi−X‾)2, S22=1m−1∑j=1m(Yj−Y‾)2S_1^2=\dfrac{1}{n-1}\sum\limits_{i=1}^n(X_i-\overline{X})^2,\ S_2^2=\dfrac{1}{m-1}\sum\limits_{j=1}^m(Y_j-\overline{Y})^2.
  2. By the property of the sample variance of a normal population: (n−1)S12σ2∼χ2(n−1)\dfrac{(n-1)S_1^2}{\sigma^2}\sim\chi^2(n-1), (m−1)S222σ2∼χ2(m−1)\dfrac{(m-1)S_2^2}{2\sigma^2}\sim\chi^2(m-1).
  3. The two samples are mutually independent, so the two χ2\chi^2 variables above are mutually independent, and their ratio follows the FF distribution: (n−1)S12/σ2(m−1)S22/(2σ2)∼F(n−1,m−1)\dfrac{(n-1)S_1^2/\sigma^2}{(m-1)S_2^2/(2\sigma^2)}\sim F(n-1,m-1).
  4. Rearranging gives 2S12S22∼F(n−1,m−1)\dfrac{2S_1^2}{S_2^2}\sim F(n-1,m-1), so (D) is the correct choice.

Answer:

2S12S22∼F(n−1,m−1)\dfrac{2S_1^2}{S_2^2}\sim F(n-1,m-1), so (D) is the correct choice.

10. Let X1,X2X_1,X_2 be a simple random sample from the population N(μ,σ2)N(\mu,\sigma^2), where σ(σ>0)\sigma(\sigma>0) is an unknown parameter. If σ^=a∣X1−X2∣\hat{\sigma}=a|X_1-X_2| is an unbiased estimator of σ\sigma, then a=a=( )

(A) π2\frac{\sqrt{\pi}}{2}

(B) 2π2\frac{\sqrt{2\pi}}{2}

(C) π\sqrt{\pi}

(D) 2π\sqrt{2\pi}

normal distributionunbiased estimatorintegral calculation

Approach:

This question tests the use of a sample statistic as an unbiased estimator for a normal population. Unbiasedness requires E(σ^)=σE(\hat\sigma)=\sigma, so it is enough to compute E∣X1−X2∣E|X_1-X_2| in order to determine the constant aa.

Steps:

  1. Since X1,X2X_1,X_2 are independent and identically distributed, Y=X1−X2∼N(0,2σ2)Y=X_1-X_2\sim N(0,2\sigma^2), whose density is f(y)=12π2 σe−y24σ2f(y)=\dfrac{1}{\sqrt{2\pi}\sqrt2\,\sigma}e^{-\frac{y^2}{4\sigma^2}}.
  2. Computing the absolute expectation: E∣Y∣=∫−∞+∞∣y∣f(y)dy=22π2 σ∫0+∞ye−y24σ2dyE|Y|=\int_{-\infty}^{+\infty}|y|f(y)dy=\dfrac{2}{\sqrt{2\pi}\sqrt2\,\sigma}\int_0^{+\infty}ye^{-\frac{y^2}{4\sigma^2}}dy.
  3. Here ∫0+∞ye−y24σ2dy=2σ2\int_0^{+\infty}ye^{-\frac{y^2}{4\sigma^2}}dy=2\sigma^2, so E∣Y∣=4σ22π2 σ=2σπE|Y|=\dfrac{4\sigma^2}{\sqrt{2\pi}\sqrt2\,\sigma}=\dfrac{2\sigma}{\sqrt\pi}.
  4. From unbiasedness E(σ^)=aE∣Y∣=σE(\hat\sigma)=aE|Y|=\sigma we get a=π2a=\dfrac{\sqrt\pi}{2}, so (A) is the correct choice.

Answer:

a=π2a=\dfrac{\sqrt{\pi}}{2}, so (A) is the correct choice.

Part II: Fill in the Blank

Part II: Fill in the Blank: Questions 11-16, 5 points each, 30 points in total.

11. As x→0x\to0, the functions f(x)=ax+bx2+ln⁡(1+x)f(x)=ax+bx^2+\ln(1+x) and g(x)=ex2−cos⁡xg(x)=e^{x^2}-\cos x are equivalent infinitesimals, then ab=ab=____.

equivalent infinitesimalTaylor expansionlimit calculation

Approach:

This question tests the definition of equivalent infinitesimals and Taylor expansions. That f(x)f(x) and g(x)g(x) are equivalent means that their ratio tends to 1, and comparing the coefficients of the linear and the quadratic terms determines a,ba,b.

Steps:

  1. From ln⁡(1+x)=x−x22+o(x2)\ln(1+x)=x-\dfrac{x^2}{2}+o(x^2) we get f(x)=ax+bx2+ln⁡(1+x)=(a+1)x+(b−12)x2+o(x2)f(x)=ax+bx^2+\ln(1+x)=(a+1)x+\left(b-\dfrac12\right)x^2+o(x^2).
  2. From ex2=1+x2+o(x2)e^{x^2}=1+x^2+o(x^2) and cos⁡x=1−x22+o(x2)\cos x=1-\dfrac{x^2}{2}+o(x^2) we get g(x)=32x2+o(x2)g(x)=\dfrac32x^2+o(x^2).
  3. Equivalent infinitesimals require lim⁡x→0f(x)g(x)=1\lim\limits_{x\to0}\dfrac{f(x)}{g(x)}=1: the coefficient of the linear term must vanish, that is a+1=0a+1=0, which gives a=−1a=-1.
  4. The coefficients of the quadratic terms are equal, that is b−12=32b-\dfrac12=\dfrac32, which gives b=2b=2.
  5. Hence ab=−2ab=-2.

Answer:

ab=−2ab=-2.

12. The equation of the tangent plane to the surface z=x+2y+ln⁡(1+x2+y2)z=x+2y+\ln(1+x^2+y^2) at the point (0,0,0)(0,0,0) is____.

tangent planepartial derivativenormal vector

Approach:

This question tests the method of finding the tangent plane to a surface. Write the surface in implicit form F(x,y,z)=0F(x,y,z)=0, find the normal vector, and then substitute the point to obtain the equation of the tangent plane.

Steps:

  1. Put F(x,y,z)=x+2y+ln⁡(1+x2+y2)−zF(x,y,z)=x+2y+\ln(1+x^2+y^2)-z, then the surface is F=0F=0.
  2. The partial derivatives are Fx=1+2x1+x2+y2F_x=1+\dfrac{2x}{1+x^2+y^2}, Fy=2+2y1+x2+y2F_y=2+\dfrac{2y}{1+x^2+y^2}, Fz=−1F_z=-1.
  3. The normal vector at the point (0,0,0)(0,0,0) is (1,2,−1)(1,2,-1).
  4. The equation of the tangent plane is 1⋅(x−0)+2⋅(y−0)−1⋅(z−0)=01\cdot(x-0)+2\cdot(y-0)-1\cdot(z-0)=0, that is x+2y−z=0x+2y-z=0.

Answer:

The equation of the tangent plane is x+2y−z=0x+2y-z=0.

13. Let f(x)f(x) be a periodic function of period 2, and let f(x)=1−x,x∈[0,1]f(x)=1-x,x\in[0,1]. If

f(x)=a02+∑n=1∞ancos⁡nπxf(x)=\frac{a_0}{2}+\sum\limits_{n=1}^{\infty} a_n\cos n\pi x

then ∑n=1∞a2n=\sum\limits_{n=1}^{\infty} a_{2n}=____.

Fourier seriescosine seriesintegral calculation

Approach:

This question tests the computation of the coefficients of a Fourier cosine series and the summation of an infinite series. First ana_n is obtained from the formula, and then the sum is evaluated at the odd indices.

Steps:

  1. f(x)f(x) is expanded as a cosine series, and by the coefficient formula an=2∫01(1−x)cos⁡nπx dxa_n=2\int_0^1(1-x)\cos n\pi x\,dx.
  2. Integrating by parts: an=2(∫01cos⁡nπx dx−∫01xcos⁡nπx dx)=1nπsin⁡nπx∣01−1nπ∫01x dsin⁡nπxa_n=2\left(\int_0^1\cos n\pi x\,dx-\int_0^1x\cos n\pi x\,dx\right)=\dfrac{1}{n\pi}\sin n\pi x\Big|_0^1-\dfrac{1}{n\pi}\int_0^1x\,d\sin n\pi x.
  3. Continuing with integration by parts gives an=−2nπ([xsin⁡nπx∣01−∫01sin⁡nπx dx])=−2nπ⋅1−cos⁡nπnπa_n=-\dfrac{2}{n\pi}\left(\left[x\sin n\pi x\Big|_0^1-\int_0^1\sin n\pi x\,dx\right]\right)=-\dfrac{2}{n\pi}\cdot\dfrac{1-\cos n\pi}{n\pi}.
  4. That is an=2(cos⁡nπ−1)n2π2a_n=\dfrac{2(\cos n\pi-1)}{n^2\pi^2}.
  5. For n=2kn=2k we have cos⁡2kπ=1\cos 2k\pi=1, so a2k=0a_{2k}=0, and hence ∑n=1∞a2n=0\sum\limits_{n=1}^{\infty}a_{2n}=0.

Answer:

∑n=1∞a2n=0\sum\limits_{n=1}^{\infty}a_{2n}=0.

14. Let the continuous function f(x)f(x) satisfy f(x+2)−f(x)=xf(x+2)-f(x)=x, ∫02f(x)dx=0\int_0^2 f(x)dx=0. Then ∫03f(x)dx=\int_0^3 f(x)dx=____.

definite integralproperty of a functionintegral calculation

Approach:

This question tests the computation of a definite integral by means of the recurrence relation f(x+2)−f(x)=xf(x+2)-f(x)=x of the function. Turn ∫23f(x)dx\int_2^3f(x)dx into ∫01f(x+2)dx\int_0^1f(x+2)dx by a change of variables, and then use the recurrence relation to replace f(x+2)f(x+2) by f(x)+xf(x)+x.

Steps:

  1. ∫03f(x)dx=∫02f(x)dx+∫23f(x)dx\displaystyle\int_0^3f(x)dx=\int_0^2f(x)dx+\int_2^3f(x)dx, and the condition gives ∫02f(x)dx=0\int_0^2f(x)dx=0.
  2. By the substitution ∫23f(x)dx=∫01f(x+2)dx=∫01[f(x)+x]dx\displaystyle\int_2^3f(x)dx=\int_0^1f(x+2)dx=\int_0^1\left[f(x)+x\right]dx.
  3. Hence ∫03f(x)dx=∫02f(x)dx+∫01f(x)dx+∫01x dx=0+∫01f(x)dx+12\displaystyle\int_0^3f(x)dx=\int_0^2f(x)dx+\int_0^1f(x)dx+\int_0^1x\,dx=0+\int_0^1f(x)dx+\dfrac12.
  4. Integrating f(x+2)−f(x)=xf(x+2)-f(x)=x over [0,1][0,1] gives ∫23f(x)dx−∫01f(x)dx=∫01x dx=12\displaystyle\int_2^3f(x)dx-\int_0^1f(x)dx=\int_0^1x\,dx=\dfrac12, that is ∫23f(x)dx=∫01f(x)dx+12\displaystyle\int_2^3f(x)dx=\int_0^1f(x)dx+\dfrac12.
  5. Eliminating ∫01f(x)dx\displaystyle\int_0^1f(x)dx from the two equations gives ∫03f(x)dx=12\displaystyle\int_0^3f(x)dx=\dfrac12.

Answer:

∫03f(x)dx=12\displaystyle\int_0^3f(x)dx=\dfrac{1}{2}.

15. Given the vectors α1=(101), α2=(−101), α3=(011), β=(11−1)\alpha_1=\begin{pmatrix}1\\0\\1\end{pmatrix},\ \alpha_2=\begin{pmatrix}-1\\0\\1\end{pmatrix},\ \alpha_3=\begin{pmatrix}0\\1\\1\end{pmatrix},\ \beta=\begin{pmatrix}1\\1\\-1\end{pmatrix}, γ=k1α1+k2α2+k3α3\gamma=k_1\alpha_1+k_2\alpha_2+k_3\alpha_3, if γTαi=βTαi(i=1,2,3)\gamma^T\alpha_i=\beta^T\alpha_i(i=1,2,3), then k12+k22+k32=k_1^2+k_2^2+k_3^2=____.

inner product of vectorssystem of linear equationsvector operation

Approach:

This question tests a system of linear equations built from inner products of vectors. After the condition γTαi=βTαi (i=1,2,3)\gamma^T\alpha_i=\beta^T\alpha_i\ (i=1,2,3) is expanded it becomes a system of linear equations in the unknowns k1,k2,k3k_1,k_2,k_3, and after it is solved the sum of the squares is required.

Steps:

  1. From γTαi=βTαi\gamma^T\alpha_i=\beta^T\alpha_i we get k1α1Tαi+k2α2Tαi+k3α3Tαi=βTαi (i=1,2,3)k_1\alpha_1^T\alpha_i+k_2\alpha_2^T\alpha_i+k_3\alpha_3^T\alpha_i=\beta^T\alpha_i\ (i=1,2,3).
  2. Computing the inner products: α1Tα1=2, α2Tα1=0, α3Tα1=1\alpha_1^T\alpha_1=2,\ \alpha_2^T\alpha_1=0,\ \alpha_3^T\alpha_1=1; α2Tα2=2, α3Tα2=1\alpha_2^T\alpha_2=2,\ \alpha_3^T\alpha_2=1; α3Tα3=2\alpha_3^T\alpha_3=2; βTα1=0, βTα2=−2, βTα3=0\beta^T\alpha_1=0,\ \beta^T\alpha_2=-2,\ \beta^T\alpha_3=0.
  3. Hence the system of equations is 2k1+k3=0, 2k2+k3=−2, k1+k2+2k3=02k_1+k_3=0,\ 2k_2+k_3=-2,\ k_1+k_2+2k_3=0.
  4. Solving gives k1=−12, k2=−32, k3=1k_1=-\dfrac12,\ k_2=-\dfrac32,\ k_3=1.
  5. Hence k12+k22+k32=14+94+1k_1^2+k_2^2+k_3^2=\dfrac{1}{4}+\dfrac{9}{4}+1.

Answer:

k12+k22+k32=119k_1^2+k_2^2+k_3^2=\dfrac{11}{9}.

16. Let the random variables XX and YY be mutually independent, with X∼B(1,13),Y∼B(2,12)X\sim B(1,\frac{1}{3}),Y\sim B(2,\frac{1}{2}). Then P(X=Y)=P(X=Y)=____.

binomial distributionindependent eventsprobability calculation

Approach:

This question tests the computation of the probability that two independent binomial variables take the same value. First the possible values of X,YX,Y are written down, and then independence is used to split the joint probability into a product of the marginal probabilities.

Steps:

  1. X∼B(1,13)X\sim B\left(1,\dfrac13\right), so XX takes only the values 0,10,1, and P(X=0)=23, P(X=1)=13P(X=0)=\dfrac23,\ P(X=1)=\dfrac13.
  2. Y∼B(2,12)Y\sim B\left(2,\dfrac12\right), so YY takes the values 0,1,20,1,2, and P(Y=0)=14, P(Y=1)=12, P(Y=2)=14P(Y=0)=\dfrac14,\ P(Y=1)=\dfrac12,\ P(Y=2)=\dfrac14.
  3. XX and YY are mutually independent, so P(X=Y)=P(X=0)P(Y=0)+P(X=1)P(Y=1)P(X=Y)=P(X=0)P(Y=0)+P(X=1)P(Y=1).
  4. Substituting gives P(X=Y)=23⋅14+13⋅12=16+16=13P(X=Y)=\dfrac23\cdot\dfrac14+\dfrac13\cdot\dfrac12=\dfrac16+\dfrac16=\dfrac13.

Answer:

P(X=Y)=13P(X=Y)=\dfrac{1}{3}.

Part III: Free Response

Part III: Free Response: Questions 17-22, 70 points in total. The solutions should include verbal explanations, proof procedures or computational steps.

17. (10 points)

Let the curve y=y(x)(x>0)y=y(x)(x>0) pass through the point (1,2)(1,2), and let the distance from an arbitrary point P(x,y)P(x,y) of the curve to the yy-axis be equal to the intercept on the yy-axis of the tangent to the curve at that point.

(I) Find y(x)y(x);

(II) Find the maximum of the function f(x)=∫1xy(t)dtf(x)=\int_1^x y(t)dt on (0,+∞)(0,+\infty).

differential equationtangent equationextremum of an integral

Approach:

This question tests the establishment of a differential equation from a geometric condition and the extremum of an integral function. In the first part the statement “the intercept on the yy-axis of the tangent equals the distance from the point to the yy-axis” is turned into an equation; in the second part the integral function is differentiated to find its stationary points.

Steps:

  1. (I) Let the equation of the tangent at the point (x,y)(x,y) be y−y0=y′(x0)(x−x0)y-y_0=y'(x_0)(x-x_0); putting x=0x=0 shows that the intercept of the tangent on the yy-axis is y−xy′y-xy'.
  2. The distance from the point to the yy-axis is xx, so y−xy′=xy-xy'=x, that is y=x(y−xy′)y=x(y-xy'), which gives y=x(2−ln⁡x)y=x(2-\ln x).
  3. The curve also passes through the point (1,2)(1,2), that is y(1)=2y(1)=2, so y(x)=x(2−ln⁡x)y(x)=x(2-\ln x).
  4. (II) f(x)=∫1x(2−ln⁡t)t dtf(x)=\int_1^x(2-\ln t)t\,dt, and by the fundamental theorem of calculus f′(x)=x(2−ln⁡x)f'(x)=x(2-\ln x); setting f′(x)=0f'(x)=0 gives the stationary point x=e2x=e^2.
  5. When 0<x<e20<x<e^2 we have f′(x)>0f'(x)>0, and when x>e2x>e^2 we have f′(x)<0f'(x)<0, so ff attains its maximum at x=e2x=e^2.
  6. f(e2)=∫1e2(2−ln⁡x)x dx=14e4−54f(e^2)=\int_1^{e^2}(2-\ln x)x\,dx=\dfrac14e^4-\dfrac54.

Answer:

(I) y(x)=x(2−ln⁡x)y(x)=x(2-\ln x);

(II) the maximum of f(x)=∫1xy(t)dtf(x)=\int_1^xy(t)dt is 14e4−54\dfrac{1}{4}e^4-\dfrac{5}{4}, attained at x=e2x=e^2.

18. (12 points)

Find the extrema of the function f(x,y)=(y−x2)(y−x3)f(x,y)=(y-x^2)(y-x^3).

extremum of a multivariable functionpartial derivativesufficient condition

Approach:

This question tests the criterion for the extrema of a function of two variables. First the stationary point equations are solved, and then the determinant AC−B2AC-B^2 formed by the second partial derivatives is used to decide the case; when the determinant vanishes the criterion fails, and one has to approach along a curve to judge the sign of the function values.

Steps:

  1. The partial derivatives are fx=−2x(y−x2)−3x2(y−x3)f_x=-2x(y-x^2)-3x^2(y-x^3), fy=2y−x2−3y2+3x3f_y=2y-x^2-3y^2+3x^3; setting both equal to zero gives the stationary points (0,0)(0,0), (1,1)(1,1), (23,1027)\left(\dfrac23,\dfrac{10}{27}\right).
  2. The second partial derivatives are fxx=−(2y+3y−15x2)f_{xx}=-(2y+3y-15x^2), fxy=−(2+3x)f_{xy}=-(2+3x), fyy=2f_{yy}=2.
  3. At (0,0)(0,0) we have A=0, B=−2, C=2A=0,\ B=-2,\ C=2, AC−B2=0AC-B^2=0, so the sufficient condition fails; taking y=x2+kx3 (k>0)y=x^2+kx^3\ (k>0) gives f(x,y)=kx5+o(x5)f(x,y)=kx^5+o(x^5), and by the local sign preservation of limits the values of the function change sign near (0,0)(0,0), so it is not an extremum.
  4. At (1,1)(1,1) we have A=12, B=−5, C=2A=12,\ B=-5,\ C=2, AC−B2=24−25<0AC-B^2=24-25<0, so it is not an extremum.
  5. At (23,1027)\left(\dfrac23,\dfrac{10}{27}\right) we have A=10027, B=83, C=2A=\dfrac{100}{27},\ B=\dfrac83,\ C=2, AC−B2>0AC-B^2>0 and A>0A>0, so it is a local minimum point, and the minimum value is (1027−49)(1027−827)=−4729\left(\dfrac{10}{27}-\dfrac49\right)\left(\dfrac{10}{27}-\dfrac8{27}\right)=-\dfrac4{729}.

Answer:

(23,1027)\left(\dfrac{2}{3},\dfrac{10}{27}\right) is a local minimum point, and the minimum value is −4729-\dfrac{4}{729}; neither (0,0)(0,0) nor (1,1)(1,1) is an extremum, so the function has no extremum.

19. (12 points)

Let Ω\Omega be the bounded region of space enclosed by the cylinder x2+y2=1x^2+y^2=1 and the planes z=0z=0 and x+z=1x+z=1, and let Σ\Sigma be the outer side of Ω\Omega. Compute the surface integral

I=∬Σ2xzdxdz+xzcos⁡ydzdy+3yzsin⁡xdxdyI=\iint_{\Sigma} 2xz dx dz+xz\cos y dz dy+3yz\sin x dx dy
Gauss's formulatriple integralpolar coordinates

Approach:

This question tests the application of Gauss’s formula (the divergence theorem). A surface integral over a closed surface can be turned into the volume integral of a divergence, and the terms containing odd functions integrate to zero because of the symmetry of the region.

Steps:

  1. The vector field is F=(2xz, xzcos⁡y, 3yzsin⁡x)F=(2xz,\ xz\cos y,\ 3yz\sin x), whose divergence is div⁡F=2z−xsin⁡y+3ysin⁡x\operatorname{div}F=2z-x\sin y+3y\sin x.
  2. By Gauss’s formula I=∭Ω(2z−xsin⁡y+3ysin⁡x) dVI=\iiint_\Omega(2z-x\sin y+3y\sin x)\,dV.
  3. The region Ω\Omega is symmetric about y=0y=0 and about z=0z=0, so the two terms containing xsin⁡yx\sin y and ysin⁡xy\sin x integrate to zero, and only ∭Ω2z dV\iiint_\Omega2z\,dV is left.
  4. Integrating first with respect to zz and then over DxyD_{xy}: ∭Ω2z dV=∬Dxydx dy∫01−x2z dz=∬Dxy(1−x)2 dx dy\displaystyle\iiint_\Omega2z\,dV=\iint_{D_{xy}}dx\,dy\int_0^{1-x}2z\,dz=\iint_{D_{xy}}(1-x)^2\,dx\,dy, where Dxy:x2+y2≤1D_{xy}:x^2+y^2\le1.
  5. In polar coordinates x=rcos⁡θ, y=rsin⁡θx=r\cos\theta,\ y=r\sin\theta, 0≤r≤1, 0≤θ≤2π0\le r\le1,\ 0\le\theta\le2\pi: I=∫02πdθ∫01r(1−rcos⁡θ)2dr=π∫01r(2+r2)dr=π(1+14)=5π4\displaystyle I=\int_0^{2\pi}d\theta\int_0^1r(1-r\cos\theta)^2dr=\pi\int_0^1r(2+r^2)dr=\pi\left(1+\dfrac14\right)=\dfrac{5\pi}{4}.

Answer:

I=5π4I=\dfrac{5\pi}{4}.

20. (12 points)

Let the function f(x)f(x) have a continuous second derivative on [−a,a][-a,a]. Prove:

(I) If f(x)=0f(x)=0, then there exists ξ∈(−a,a)\xi\in(-a,a) such that f′′(ξ)=1a2[f(a)+f(−a)]f''(\xi)=\frac{1}{a^2}[f(a)+f(-a)];

(II) If f(x)f(x) attains an extremum in (−a,a)(-a,a) and f(x)f(x) is differentiable at x=x0x=x_0, then

∣f′′(η)∣≥12a2∣f(a)−f(−a)∣|f''(\eta)|\geq\frac{1}{2a^2}|f(a)-f(-a)|
Taylor formulaintermediate value theoremintegral inequality

Approach:

This question tests the application of the Taylor formula and the intermediate value theorem to an integral inequality. In the first part the expansions with the Lagrange remainder are written down at the two endpoints and added; in the second part the function is expanded once more at the extremum, and the difference is controlled by the maximum of ∣f′′∣|f''|.

Steps:

  1. (I) From f(x)=0f(x)=0 and the Taylor formula, f(a)=f′(0)a+f′′(η1)2a2 (0<η1<a)f(a)=f'(0)a+\dfrac{f''(\eta_1)}{2}a^2\ (0<\eta_1<a), f(−a)=−f′(0)a+f′′(η2)2a2 (−a<η2<0)f(-a)=-f'(0)a+\dfrac{f''(\eta_2)}{2}a^2\ (-a<\eta_2<0).
  2. Adding the two equations gives f(a)+f(−a)=a22[f′′(η1)+f′′(η2)]f(a)+f(-a)=\dfrac{a^2}{2}\left[f''(\eta_1)+f''(\eta_2)\right].
  3. By the continuity of f′′f'' and the intermediate value theorem there exists ξ∈(−a,a)\xi\in(-a,a) with f′′(ξ)=f′′(η1)+f′′(η2)2f''(\xi)=\dfrac{f''(\eta_1)+f''(\eta_2)}{2}, hence f′′(ξ)=1a2[f(a)+f(−a)]f''(\xi)=\dfrac{1}{a^2}\left[f(a)+f(-a)\right].
  4. (II) Suppose ff attains an extremum at x0∈(−a,a)x_0\in(-a,a) and is differentiable there, so f′(x0)=0f'(x_0)=0. By the Taylor formula f(−a)=f(x0)+f′′(γ1)2(−a−x0)2f(-a)=f(x_0)+\dfrac{f''(\gamma_1)}{2}(-a-x_0)^2, f(a)=f(x0)+f′′(γ2)2(a−x0)2f(a)=f(x_0)+\dfrac{f''(\gamma_2)}{2}(a-x_0)^2.
  5. Subtracting the two equations gives f(a)−f(−a)=12[(a−x0)2f′′(γ2)−(a+x0)2f′′(γ1)]f(a)-f(-a)=\dfrac12\left[(a-x_0)^2f''(\gamma_2)-(a+x_0)^2f''(\gamma_1)\right].
  6. Put M=max⁡{∣f′′(γ1)∣, ∣f′′(γ2)∣}M=\max\{|f''(\gamma_1)|,\ |f''(\gamma_2)|\}; then ∣f(a)−f(−a)∣≤M2[(a−x0)2+(a+x0)2]=M(a2+x02)≤2Ma2|f(a)-f(-a)|\le\dfrac M2\left[(a-x_0)^2+(a+x_0)^2\right]=M(a^2+x_0^2)\le2Ma^2, so ∣f′′(η)∣≥12a2∣f(a)−f(−a)∣|f''(\eta)|\ge\dfrac{1}{2a^2}|f(a)-f(-a)|.

Answer:

(I) there exists ξ∈(−a,a)\xi\in(-a,a) with f′′(ξ)=1a2[f(a)+f(−a)]f''(\xi)=\dfrac{1}{a^2}\left[f(a)+f(-a)\right];

(II) there exists η∈(−a,a)\eta\in(-a,a) with ∣f′′(η)∣≥12a2∣f(a)−f(−a)∣|f''(\eta)|\geq\dfrac{1}{2a^2}|f(a)-f(-a)|.

21. (12 points)

Given the quadratic forms f(x1,x2,x3)=x12+2x22+2x32+2x1x2+2x2x3−2x1x3f(x_1,x_2,x_3)=x_1^2+2x_2^2+2x_3^2+2x_1x_2+2x_2x_3-2x_1x_3,

g(y1,y2,y3)=y12+y22+y32+2y2y3g(y_1,y_2,y_3)=y_1^2+y_2^2+y_3^2+2y_2y_3.

(I) Find an invertible transformation x=Pyx=Py that turns f(x1,x2,x3)f(x_1,x_2,x_3) into g(y1,y2,y3)g(y_1,y_2,y_3);

(II) Does there exist an orthogonal transformation x=Qyx=Qy that turns f(x1,x2,x3)f(x_1,x_2,x_3) into g(y1,y2,y3)g(y_1,y_2,y_3)?

quadratic formcompleting the squareorthogonal transformation

Approach:

This question tests the method of completing the square for a quadratic form and the criterion for congruence. First both quadratic forms are reduced to their canonical forms, which establishes the invertible transformation; then the rank of the matrices is used to decide whether an orthogonal transformation exists.

Steps:

  1. (I) Completing the square for ff: f(x1,x2,x3)=(x1+x2−x3)2+(x2+x3)2f(x_1,x_2,x_3)=(x_1+x_2-x_3)^2+(x_2+x_3)^2.
  2. Put z1=x1+x2−x3, z2=x2+x3, z3=x3z_1=x_1+x_2-x_3,\ z_2=x_2+x_3,\ z_3=x_3, then (z1z2z3)=(11−1011001)(x1x2x3)\begin{pmatrix}z_1\\z_2\\z_3\end{pmatrix}=\begin{pmatrix}1&1&-1\\0&1&1\\0&0&1\end{pmatrix}\begin{pmatrix}x_1\\x_2\\x_3\end{pmatrix}, which gives f=z12+z22f=z_1^2+z_2^2.
  3. Completing the square for gg: g(y1,y2,y3)=y12+(y2+y3)2g(y_1,y_2,y_3)=y_1^2+(y_2+y_3)^2. Put z1=y1, z2=y2+y3, z3=y3z_1=y_1,\ z_2=y_2+y_3,\ z_3=y_3, then (z1z2z3)=(100011001)(y1y2y3)\begin{pmatrix}z_1\\z_2\\z_3\end{pmatrix}=\begin{pmatrix}1&0&0\\0&1&1\\0&0&1\end{pmatrix}\begin{pmatrix}y_1\\y_2\\y_3\end{pmatrix}, which gives g=z12+z22g=z_1^2+z_2^2.
  4. Comparing the two transformations gives (x1x2x3)=P(y1y2y3)\begin{pmatrix}x_1\\x_2\\x_3\end{pmatrix}=P\begin{pmatrix}y_1\\y_2\\y_3\end{pmatrix}, where P=(11−1011001)P=\begin{pmatrix}1&1&-1\\0&1&1\\0&0&1\end{pmatrix}.
  5. (II) The matrices of ff and gg are A=(11−1120−102)A=\begin{pmatrix}1&1&-1\\1&2&0\\-1&0&2\end{pmatrix} and B=(100011011)B=\begin{pmatrix}1&0&0\\0&1&1\\0&1&1\end{pmatrix} respectively. If an orthogonal transformation x=Qyx=Qy exists, then QTAQ=Q−1AQ=BQ^TAQ=Q^{-1}AQ=B, that is AA and BB are similar.
  6. But r(A)=5≠3=r(B)r(A)=5\ne3=r(B), so the two are not similar and hence no such orthogonal transformation exists.

Answer:

(I) P=(11−1011001)P=\begin{pmatrix}1&1&-1\\0&1&1\\0&0&1\end{pmatrix};

(II) no orthogonal transformation x=Qyx=Qy exists.

22. (12 points)

Let the probability density of the two-dimensional random variable (X,Y)(X,Y) be

f(x,y)={2π(x2+y2),x2+y2≤10,otherf(x,y)=\begin{cases}\frac{2}{\pi}(x^2+y^2), & x^2+y^2\leq1\\0, & \text{other}\end{cases}

(I) Find the variances of xx and yy;

(II) Determine whether xx and yy are mutually independent;

(III) Find the probability density of z=x2+y2z=x^2+y^2.

probability densitymarginal distributiontransformation of random variables

Approach:

This question tests the moments, the marginal distributions and the distribution of a function of a random variable of a two-dimensional random variable. First the moments are computed in polar coordinates and the marginal densities are found in order to decide independence; then the distribution function method is used to find the density of z=x2+y2z=x^2+y^2.

Steps:

  1. (I) E(X)=∬Dx2π(x2+y2)dσ=0E(X)=\iint_D x\dfrac{2}{\pi}(x^2+y^2)d\sigma=0 (the region is symmetric about the yy-axis), E(X2)=∬Dx22π(x2+y2)dσ=13E(X^2)=\iint_Dx^2\dfrac{2}{\pi}(x^2+y^2)d\sigma=\dfrac13, hence D(X)=13D(X)=\dfrac13, and similarly D(Y)=13D(Y)=\dfrac13.
  2. (II) The marginal densities are: fX(x)=∫−1−x21−x22π(x2+y2)dy=43π(1+2x2)1−x2f_X(x)=\int_{-\sqrt{1-x^2}}^{\sqrt{1-x^2}}\dfrac{2}{\pi}(x^2+y^2)dy=\dfrac{4}{3\pi}(1+2x^2)\sqrt{1-x^2}, and similarly fY(y)=43π(1+2y2)1−y2f_Y(y)=\dfrac{4}{3\pi}(1+2y^2)\sqrt{1-y^2}.
  3. Since fX(x)fY(y)≠f(x,y)f_X(x)f_Y(y)\ne f(x,y), XX and YY are not mutually independent.
  4. (III) FZ(z)=P(x2+y2≤z)F_Z(z)=P(x^2+y^2\le z): it is 0 when z<0z<0; when 0≤z<10\le z<1 we have FZ(z)=∬Dz2π(x2+y2)dσ=2π∫02πdθ∫0zr3dr=z2F_Z(z)=\iint_{D_z}\dfrac{2}{\pi}(x^2+y^2)d\sigma=\dfrac{2}{\pi}\int_0^{2\pi}d\theta\int_0^{\sqrt z}r^3dr=z^2; and it is 1 when z≥1z\ge1.
  5. Differentiating gives fZ(z)={2z,0<z<1,0,other.f_Z(z)=\begin{cases}2z, & 0<z<1,\\0, & \text{other}.\end{cases}

Answer:

(I) D(X)=D(Y)=13D(X)=D(Y)=\dfrac{1}{3};

(II) XX and YY are not mutually independent;

(III) fZ(z)={2z,0<z<1,0,otherf_Z(z)=\begin{cases}2z, & 0<z<1,\\0, & \text{other}\end{cases}.

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