The force exerted by the water jet is equal to the force exerted on the spring due to the deflection. The spring force is given by:
\[
F_{\text{spring}} = k \times \delta
\]
Where:
- \( k = 1 \ \text{kN/m} = 1000 \ \text{N/m} \) is the spring constant,
- \( \delta = 1 \ \text{cm} = 0.01 \ \text{m} \) is the deflection.
Thus, the spring force is:
\[
F_{\text{spring}} = 1000 \times 0.01 = 10 \ \text{N}
\]
This force is due to the momentum of the incoming jet. The force due to the jet is given by:
\[
F_{\text{jet}} = \dot{m} \cdot v
\]
Where:
- \( \dot{m} = \rho \cdot A \cdot v \) is the mass flow rate,
- \( \rho = 1000 \ \text{kg/m}^3 \) is the density of water,
- \( A = \pi \left(\frac{D}{2}\right)^2 \) is the cross-sectional area of the jet,
- \( v \) is the velocity of the jet.
Substitute the values for \( A \) and \( \dot{m} \):
\[
A = \pi \left(\frac{0.01}{2}\right)^2 = 7.854 \times 10^{-5} \ \text{m}^2
\]
\[
\dot{m} = 1000 \times 7.854 \times 10^{-5} \times v = 0.07854 \times v
\]
Now, equating the spring force and jet force:
\[
10 = 0.07854 \times v^2
\]
Solving for \( v \):
\[
v^2 = \frac{10}{0.07854} = 127.4
\]
\[
v = \sqrt{127.4} \approx 11.3 \ \text{m/s}
\]
Thus, the velocity of the incoming jet is:
\[
\boxed{11.3 \ \text{m/s}}
\]