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Step 1: Interpret the conditions We are told: - \( Q^{-1} = Q^T \) $\Rightarrow $ \( Q \) is an orthogonal matrix
. - \( Q \) is invertible with integer entries $\Rightarrow$ entries must be from \(−1, 0, 1\).
- \( PQ = QP \) $\Rightarrow$ \( Q \) commutes with the diagonal matrix \( P \).
Step 2: Structure of \( Q \) The matrix \( P \) has eigenvalues 2, 2, and 3. This means the eigenspace corresponding to 2 is 2-dimensional (spanned by standard basis vectors \( e_1, e_2 \)), and the eigenspace corresponding to 3 is 1-dimensional (spanned by \( e_3 \)).
Since \( Q \) must commute with \( P \), it must preserve these eigenspaces. So \( Q \) must be of the form: \[ Q = \begin{pmatrix} Q_1 & 0
0 & \pm 1 \end{pmatrix} \] where \( Q_1 \) is a \( 2 \times 2 \) orthogonal matrix with integer entries.
Step 3: Count such matrices The number of \( 2 \times 2 \) orthogonal matrices over integers is 4 (rotations and reflections in 2D with integer entries): - Identity, swap rows, sign flips, etc. And for the bottom-right corner (\( \pm1 \)), we have 2 choices. So total number of such matrices: \[ 4 \times 2 = \boxed{8} \]
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 