
To solve the problem, we need to find the observed frequency when the observer and the source move away from each other.
1. Given Data:
The original frequency of the source is $f_0 = 240 \, \text{Hz}$.
The speed of the observer and the source with respect to the ground is $v$.
The speed of sound in air is $V$.
2. Case 1 - Moving Towards Each Other:
In Case 1, the observer and the source move towards each other, so the observed frequency is:
$ f_1 = f_0 \frac{V+v}{V-v} = 288 \, \text{Hz}$
3. Solving for $v$:
We have:
$ \frac{V+v}{V-v} = \frac{288}{240} = \frac{6}{5}$
Multiplying both sides by $5(V-v)$ gives:
$ 5(V+v) = 6(V-v)$
Expanding the terms gives:
$ 5V + 5v = 6V - 6v$
Combining like terms:
$ 11v = V$
Therefore, $v = \frac{V}{11}$.
4. Case 2 - Moving Away From Each Other:
In Case 2, the observer and the source move away from each other, so the observed frequency is:
$ f_2 = f_0 \frac{V-v}{V+v} = n \, \text{Hz}$
5. Substituting $v = \frac{V}{11}$ into the Formula:
We have:
$ n = 240 \frac{V - \frac{V}{11}}{V + \frac{V}{11}}$
This simplifies to:
$ n = 240 \frac{\frac{10V}{11}}{\frac{12V}{11}} = 240 \times \frac{10}{12} = 240 \times \frac{5}{6} = 200$
Final Answer:
The final answer is $\boxed{200}$.
To solve this Doppler effect problem, we use the formulas for frequency observed when the source and observer move towards and away from each other.
Given:
- Source frequency \( f = 240 \, \text{Hz} \)
- Observed frequency when moving towards each other \( f' = 288 \, \text{Hz} \)
- Observed frequency when moving away \( f'' = n \, \text{Hz} \) (to be found)
- Speed of sound in air \( v_s \) (assumed constant)
- Speed of source and observer relative to ground = \( v \)
Step 1: Doppler effect formula
When source and observer move towards each other with speed \( v \):
\[
f' = f \frac{v_s + v}{v_s - v}
\]
When source and observer move away from each other with speed \( v \):
\[
f'' = f \frac{v_s - v}{v_s + v}
\]
Step 2: Use the given values to find \( v_s \) and \( v \)
From the towards case:
\[
288 = 240 \cdot \frac{v_s + v}{v_s - v}
\]
Simplify:
\[
\frac{288}{240} = 1.2 = \frac{v_s + v}{v_s - v}
\]
Cross-multiplied:
\[
1.2 (v_s - v) = v_s + v
\]
\[
1.2 v_s - 1.2 v = v_s + v
\]
\[
1.2 v_s - v_s = v + 1.2 v
\]
\[
0.2 v_s = 2.2 v
\]
\[
v = \frac{0.2}{2.2} v_s = \frac{1}{11} v_s
\]
Step 3: Find \( n = f'' \)
Using the away formula:
\[
n = 240 \times \frac{v_s - v}{v_s + v} = 240 \times \frac{1 - \frac{1}{11}}{1 + \frac{1}{11}} = 240 \times \frac{\frac{10}{11}}{\frac{12}{11}} = 240 \times \frac{10}{12} = 240 \times \frac{5}{6} = 200
\]
Final Answer:
\[
\boxed{n = 200 \text{ Hz}}
\]
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): 
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 ________.