Step 1: Understanding the Question:
The question relates the speed of sound in a gas to its temperature. We are given the speed at \(0^\circ C\) and are told it doubles at a new temperature \(\alpha^\circ C\). We need to find \(\alpha\).
Step 2: Key Formula or Approach:
The speed of sound (\(V\)) in an ideal gas is proportional to the square root of its absolute temperature (\(T\)).
\[ V = \sqrt{\frac{\gamma R T}{M}} \]
This implies that \(V \propto \sqrt{T}\). Therefore, we can write the relation:
\[ \frac{V_1}{V_2} = \sqrt{\frac{T_1}{T_2}} \]
where \(T_1\) and \(T_2\) are in Kelvin.
Step 3: Detailed Explanation:
First, convert the given temperatures to the absolute scale (Kelvin). Remember, \(T(K) = T(^\circ C) + 273\).
- Initial temperature: \(T_1 = 0^\circ C = 0 + 273 = 273\) K.
- Final temperature: \(T_2 = \alpha^\circ C = \alpha + 273\) K.
The speeds are given as:
- Initial speed: \(V_1 = V_0\).
- Final speed: \(V_2 = 2V_0\).
Now, substitute these values into the ratio formula:
\[ \frac{V_0}{2V_0} = \sqrt{\frac{273}{\alpha + 273}} \]
\[ \frac{1}{2} = \sqrt{\frac{273}{\alpha + 273}} \]
To solve for \(\alpha\), we square both sides of the equation:
\[ \left(\frac{1}{2}\right)^2 = \frac{273}{\alpha + 273} \]
\[ \frac{1}{4} = \frac{273}{\alpha + 273} \]
Now, cross-multiply to solve for \(\alpha\):
\[ \alpha + 273 = 4 \times 273 \]
\[ \alpha = (4 \times 273) - 273 \]
\[ \alpha = 3 \times 273 \]
\[ \alpha = 819 \]
Step 4: Final Answer:
The value of \(\alpha\) is 819. Since the final temperature was given as \(\alpha^\circ C\), the answer is \(819^\circ C\).