We are given that a closed organ pipe is partially filled with water by \( \frac{1}{5} \) of its volume. We are to find how the frequency of its fundamental note changes.
The fundamental frequency of a closed organ pipe (one end closed, one end open) is given by:
\[ f = \frac{v}{4L} \]
where \( v \) is the speed of sound in air and \( L \) is the effective length of the air column. When water fills part of the pipe, the effective length of the air column decreases, and hence the frequency increases because \( f \propto \frac{1}{L} \).
Step 1: Let the total length of the pipe be \( L \).
Since the pipe is filled with water by \( \frac{1}{5} \) of its volume, the air column length becomes:
\[ L' = L - \frac{L}{5} = \frac{4L}{5} \]
Step 2: Write the new frequency of the fundamental note after filling with water.
\[ f' = \frac{v}{4L'} \] \[ f' = \frac{v}{4 \times \frac{4L}{5}} = \frac{5v}{16L} \]
Step 3: Write the ratio of the new frequency to the original frequency.
\[ \frac{f'}{f} = \frac{\frac{5v}{16L}}{\frac{v}{4L}} = \frac{5}{16} \times 4 = \frac{5}{4} \]
Step 4: Hence, the new frequency is \( \frac{5}{4} \) times the original frequency.
The frequency increases by a factor of \( \frac{5}{4} \), i.e. by 25%.
\[ \boxed{\text{The fundamental frequency increases by } 25\%} \]
Let \( \alpha = \dfrac{-1 + i\sqrt{3}}{2} \) and \( \beta = \dfrac{-1 - i\sqrt{3}}{2} \), where \( i = \sqrt{-1} \). If
\[ (7 - 7\alpha + 9\beta)^{20} + (9 + 7\alpha - 7\beta)^{20} + (-7 + 9\alpha + 7\beta)^{20} + (14 + 7\alpha + 7\beta)^{20} = m^{10}, \] then the value of \( m \) is ___________.