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 ________.
Step 1: Understanding the Problem
We are given that:
\[(1 + \frac{2}{5}x)^{23} = \sum_{i=0}^{23} a_i x^i\]
This means that \(a_i\) represents the coefficient of \(x^i\) in the expansion of \((1 + \frac{2}{5}x)^{23}\).
Step 2: General Term of the Expansion
From the binomial theorem, the general term is:
\[T_{i} = \binom{23}{i} \left(\frac{2}{5}x\right)^i\]
So, the coefficient of \(x^i\) is:
\[a_i = \binom{23}{i}\left(\frac{2}{5}\right)^i\]
Step 3: Behavior of Coefficients
We need to find which \(a_i\) is the largest among \(a_0, a_1, \dots, a_{23}\).
To do this, consider the ratio:
\[\frac{a_{i+1}}{a_i} = \frac{\binom{23}{i+1}\left(\frac{2}{5}\right)^{i+1}}{\binom{23}{i}\left(\frac{2}{5}\right)^i}\]
Simplify:
\[\frac{a_{i+1}}{a_i} = \frac{23-i}{i+1} \cdot \frac{2}{5}\]
Step 4: Condition for Increasing Sequence
If \(\frac{a_{i+1}}{a_i} > 1\), the sequence increases; if less than 1, it decreases.
\[\frac{23-i}{i+1} \cdot \frac{2}{5} > 1\]
\[\frac{23-i}{i+1} > \frac{5}{2}\]
\[2(23-i) > 5(i+1)\]
\[46 - 2i > 5i + 5\]
\[46 - 5 > 7i\]
\[41 > 7i\]
\[i < \frac{41}{7} \approx 5.857\]
Step 5: Identifying the Maximum
Thus, the coefficients increase up to \(i = 5\) and then start decreasing after \(i = 6\)
Therefore, the largest coefficient occurs at \(i = 6\).
Final Answer
The value of \(r\) is:
r = 6
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): 