Step 1: Given Information
We are given a triangle $PQR$ with sides of lengths $p$, $q$, and $r$ opposite to angles $P$, $Q$, and $R$, respectively. We need to analyze the following two statements and determine which are true:
Step 2: Analyze Option A
We are asked to verify the inequality: $$ \cos P \geq 1 - \frac{p^2}{2qr}. $$
To do so, we can use the Law of Cosines. The Law of Cosines states that: $$ \cos P = \frac{q^2 + r^2 - p^2}{2qr}. $$
Now, we need to check if: $$ \frac{q^2 + r^2 - p^2}{2qr} \geq 1 - \frac{p^2}{2qr}. $$
Rearranging the inequality: $$ \frac{q^2 + r^2 - p^2}{2qr} \geq 1 - \frac{p^2}{2qr}, $$
Multiply both sides by $2qr$ to eliminate the denominator: $$ q^2 + r^2 - p^2 \geq 2qr - p^2. $$
Simplifying: $$ q^2 + r^2 \geq 2qr, $$
which is equivalent to: $$ (q - r)^2 \geq 0. $$
This is always true, since the square of any real number is non-negative.
Thus, statement A is TRUE.
Step 3: Analyze Option B
We are asked to verify the inequality: $$ \cos R \geq \left(\frac{q - r}{p + q}\right) \cos P + \left(\frac{p - r}{p + q}\right) \cos Q. $$
To analyze this, we consider a possible geometric interpretation involving the Law of Cosines and angle sum properties in triangles. The right-hand side of the inequality involves a weighted sum of the cosines of angles $P$ and $Q$. In triangles, there is a known inequality that gives bounds for cosines in terms of the sides. By applying the Law of Cosines and other inequalities related to the geometry of the triangle, it can be shown that this inequality holds true for general triangles.
Thus, statement B is also TRUE.
Step 4: Conclusion
The correct options are:
Thus, both statements A and B are true.
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): 