Step 1: Write the formula for the fundamental frequency of a closed pipe.
A tube closed at one end (a closed organ pipe) supports standing waves where the closed end is a node and the open end is an antinode.
The fundamental frequency ($f_c$) for a pipe of length $L$ is given by:
\[
f_c = \frac{v}{4L},
\]
where $v$ is the speed of sound in air.
Step 2: Use the given beat frequency information for the closed pipes.
Let the two tubes have lengths $L_1$ and $L_2$, and their fundamental frequencies be $f_{c1}$ and $f_{c2}$.
\[
f_{c1} = \frac{v}{4L_1}, f_{c2} = \frac{v}{4L_2}.
\]
The number of beats per second is the difference in their frequencies:
\[
|f_{c1} - f_{c2}| = 2 \text{ Hz}.
\]
Step 3: Write the formula for the fundamental frequency of an open pipe.
A tube open at both ends (an open organ pipe) supports standing waves where both ends are antinodes.
The fundamental frequency ($f_o$) for a pipe of length $L$ is given by:
\[
f_o = \frac{v}{2L}.
\]
Step 4: Relate the fundamental frequencies of open and closed pipes.
For a pipe of the same length $L$, we can see the relationship between the two types of fundamental frequencies:
\[
f_o = \frac{v}{2L} = 2 \left(\frac{v}{4L}\right) = 2f_c.
\]
The fundamental frequency of an open pipe is twice the fundamental frequency of a closed pipe of the same length.
Step 5: Calculate the new beat frequency for the open pipes.
When both tubes are open at both ends, their new fundamental frequencies will be $f_{o1}$ and $f_{o2}$.
\[
f_{o1} = 2f_{c1}, f_{o2} = 2f_{c2}.
\]
The new beat frequency will be the difference between these new frequencies:
\[
\text{Beats}_{new} = |f_{o1} - f_{o2}| = |2f_{c1} - 2f_{c2}|.
\]
\[
\text{Beats}_{new} = 2|f_{c1} - f_{c2}|.
\]
Substituting the original beat frequency:
\[
\text{Beats}_{new} = 2 \times (2 \text{ Hz}) = 4 \text{ Hz}.
\]
The number of beats produced per second is 4.