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:
\[
\boxed{n = 200 \text{ Hz}}
\]
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____