Step 1: Write the two frequency conditions.
An open pipe of length $L_o$ has harmonics $f_n = \dfrac{nv}{2L_o}$, so its second harmonic is just $f_2 = \dfrac{v}{L_o}$. A closed pipe of length $L_c$ has only its fundamental, $f_1 = \dfrac{v}{4L_c}$.
Step 2: Match the two given frequencies.
We are told the open pipe's second harmonic equals the closed pipe's fundamental, so
\[
\frac{v}{L_o} = \frac{v}{4L_c}
\]
The speed of sound cancels straight away, leaving a simple length relation: $4L_c = L_o$.
Step 3: Plug in the open pipe length.
With $L_o = 80\ \text{cm}$,
\[
L_c = \frac{80}{4} = 20\ \text{cm}
\]
\[
\boxed{20\ \text{cm}}
\]