The total flow rate of water leaving the pipe is the product of the total velocity and the cross-sectional area of the pipe:
\[
Q_{\text{total}} = A \cdot V_{\text{out}},
\]
where:
- \( A = \pi \left(\frac{D}{2}\right)^2 = \pi \left(\frac{0.32}{2}\right)^2 = 0.0804 \, \text{m}^2 \) is the cross-sectional area of the pipe,
- \( V_{\text{out}} = 6 \, \text{m/s} \) is the velocity of water leaving the pipe.
Thus, the total flow rate is:
\[
Q_{\text{total}} = 0.0804 \times 6 = 0.4824 \, \text{m}^3/\text{s} = 482.4 \, \text{L/s}.
\]
The flow rate of the jet entering the pipe is:
\[
Q_{\text{in}} = A_{\text{jet}} \cdot V_{\text{in}} = 0.01 \cdot 35 = 0.35 \, \text{m}^3/\text{s} = 350 \, \text{L/s}.
\]
The flow rate of entrained water is:
\[
Q_{\text{entrained}} = Q_{\text{total}} - Q_{\text{in}} = 482.4 - 350 = 132.4 \, \text{L/s}.
\]
Thus, the flow rate of entrained water is:
\[
\boxed{130.00 \, \text{to} \, 134.00 \, \text{L/s}}.
\]