Step 1: Apply the Thiem equation for unconfined aquifers.
The Thiem equation for steady-state pumping in an unconfined aquifer is:
\[
Q = 2 \pi K \cdot H \cdot \frac{\Delta h}{\ln(r_2/r_1)}
\]
where:
\( Q \) = pumping rate (m\(^3\)/day),
\( K \) = hydraulic conductivity (10 m/day),
\( H \) = saturated thickness of the aquifer (20 m),
\( \Delta h \) = difference in drawdowns between two observation wells,
\( r_1 \) and \( r_2 \) = radial distances of the observation wells from the pumping well (10 m and 100 m, respectively).
Step 2: Substitute the given values.
From the problem:
\[
\Delta h = (5 - 1) = 4 \, \text{m}, \quad r_1 = 10 \, \text{m}, \quad r_2 = 100 \, \text{m}, \quad K = 10 \, \text{m/day}, \quad H = 20 \, \text{m}.
\]
Substitute into the Thiem equation:
\[
Q = 2 \pi (10) (20) \cdot \frac{4}{\ln(100/10)}.
\]
Step 3: Simplify the equation.
First, calculate the logarithmic term:
\[
\ln\left(\frac{100}{10}\right) = \ln(10) \approx 2.3026.
\]
Now, substitute this value:
\[
Q = 2 \pi (10) (20) \cdot \frac{4}{2.3026}.
\]
Simplify further:
\[
Q = 2 \pi (200) \cdot \frac{4}{2.3026}.
\]
\[
Q \approx 400 \pi \cdot 1.737 \approx 400 \cdot 3.1416 \cdot 1.737.
\]
Step 4: Final calculation.
\[
Q \approx 400 \cdot 5.459 \approx 1858.00 \, \text{m\(^3\)/day}.
\]
Conclusion: The corresponding pumping rate is approximately \( 1858.00 \, \text{m\(^3\)/day} \).