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CIE 9231 2025 June Paper 23 Q8

A Level / CIE / FP2

CIE 9231 2025 June Paper 23 Paper · Question 8

题目

Problem

(a) Find the values of aa for which the system of equations

32x+3y+8z= 1,ax+3y+4z= 2,ay−z= 3,\begin{align*} \frac{3}{2}x+3y+8z=&\,1,\\ ax+3y+4z=&\,2,\\ ay-z=&\,3, \end{align*}

does not have a unique solution.

(3)

The matrix A\mathbf{A} is given by

A=(323803400−1).\mathbf{A}=\begin{pmatrix}\frac{3}{2}&3&8\\0&3&4\\0&0&-1\end{pmatrix}.

(b) Given that B=A−1\mathbf{B}=\mathbf{A}^{-1}, use the characteristic equation of A\mathbf{A} to show that B2=pI+qA\mathbf{B}^2=p\mathbf{I}+q\mathbf{A}, where pp and qq are constants to be determined.

(4)

(c) Find a matrix P\mathbf{P} and a diagonal matrix D\mathbf{D} such that A−1=PDP−1\mathbf{A}^{-1}=\mathbf{P}\mathbf{D}\mathbf{P}^{-1}.

(7)
题目中文翻译

(a) 求使方程组

32x+3y+8z= 1,ax+3y+4z= 2,ay−z= 3\begin{align*} \frac{3}{2}x+3y+8z=&\,1,\\ ax+3y+4z=&\,2,\\ ay-z=&\,3 \end{align*}

没有唯一解的 aa 的值。

(3)

矩阵 A\mathbf{A} 为

A=(323803400−1).\mathbf{A}=\begin{pmatrix}\frac{3}{2}&3&8\\0&3&4\\0&0&-1\end{pmatrix}.

(b) 已知 B=A−1\mathbf{B}=\mathbf{A}^{-1},利用 A\mathbf{A} 的特征方程证明 B2=pI+qA\mathbf{B}^2=p\mathbf{I}+q\mathbf{A},其中 pp 和 qq 是待求的常数。

(4)

(c) 求矩阵 P\mathbf{P} 和对角矩阵 D\mathbf{D},使得 A−1=PDP−1\mathbf{A}^{-1}=\mathbf{P}\mathbf{D}\mathbf{P}^{-1}。

(7)
原卷通用作答要求

Answer all questions. You should use a calculator where appropriate.

You must show all necessary working clearly; no marks will be given for unsupported answers from a calculator.

Give non-exact numerical answers correct to 3 significant figures, or 1 decimal place for angles in degrees, unless a different level of accuracy is specified in the question.

请回答所有题目。适当时应使用计算器。必须清楚展示所有必要的计算过程;仅给出计算器答案而没有过程,不予评分。除非题目另有精度要求,非精确数值答案保留 3 位有效数字,以度为单位的角度保留 1 位小数。

解答

(a)

解法一

思路

展开

没有唯一解时,系数行列式为零。沿第一行展开后解关于 aa 的二次方程。

答题过程

展开

The coefficient determinant is

 det⁡(3238a340a−1)= 32(−3−4a)+3a+8a2= 8a2−3a−92.\begin{align*} &\,\det\begin{pmatrix} \frac32&3&8\\ a&3&4\\ 0&a&-1 \end{pmatrix}\\[4mm] =&\,\frac32(-3-4a)+3a+8a^2\\[4mm] =&\,8a^2-3a-\frac92. \end{align*}

The system does not have a unique solution exactly when this determinant is zero. Solving gives

a=3(1±17)16.\boxed{a=\frac{3(1\pm\sqrt{17})}{16}}.

(b)

解法一

思路

展开

用对角线上的特征值写出特征多项式。由 Cayley–Hamilton 定理得到矩阵恒等式,再乘 A−2\mathbf A^{-2}。

答题过程

展开

The characteristic polynomial of A\mathbf A is

 (λ−32)(λ−3)(λ+1)= λ3−72λ2+92.\begin{align*} &\,(\lambda-\tfrac32)(\lambda-3)(\lambda+1)\\[4mm] =&\,\lambda^3-\frac72\lambda^2+\frac92. \end{align*}

By the Cayley–Hamilton theorem,

A3−72A2+92I=0.\mathbf A^3-\frac72\mathbf A^2+\frac92\mathbf I=\mathbf0.

Multiplying by B2=A−2\mathbf B^2=\mathbf A^{-2} gives A−72I+92B2=0\mathbf A-\frac72\mathbf I+\frac92\mathbf B^2=\mathbf0. Hence

B2=79I−29A,(p,q)=(79,−29).\mathbf B^2=\frac79\mathbf I-\frac29\mathbf A, \qquad (p,q)=\bigg(\frac79,-\frac29\bigg).

(c)

解法一

思路

展开

先用 A\mathbf A 的三个特征值求特征向量。取逆时特征向量不变,特征值变为原值的倒数。

答题过程

展开

Solving (A−λI)v=0(\mathbf A-\lambda\mathbf I)\mathbf v=\mathbf0 gives the following choices.

  • For λ=32\lambda=\frac32, the second and third coordinates are zero, so take (1,0,0)T(1,0,0)^{\mathsf T}.
  • For λ=3\lambda=3, the third coordinate is zero and the first is twice the second, so take (2,1,0)T(2,1,0)^{\mathsf T}.
  • For λ=−1\lambda=-1, the equations are v2=−v3v_2=-v_3 and 52v1+3v2+8v3=0\frac52v_1+3v_2+8v_3=0, so take (2,1,−1)T(2,1,-1)^{\mathsf T}.

The corresponding eigenvalues of A−1\mathbf A^{-1} are 23,13,−1\frac23,\frac13,-1. Thus

P=(12201100−1),D=(2300013000−1)\mathbf P=\begin{pmatrix} 1&2&2\\0&1&1\\0&0&-1 \end{pmatrix}, \qquad \mathbf D=\begin{pmatrix} \frac23&0&0\\0&\frac13&0\\0&0&-1 \end{pmatrix}

give A−1=PDP−1\mathbf A^{-1}=\mathbf P\mathbf D\mathbf P^{-1}.