Hydraulic Transients: Water Hammer Dynamics and Surge Tank Mechanics
Rapid valve closure or sudden turbine shutdown in long pressure conduits (penstocks) induces severe pressure oscillations known as Water Hammer. The instantaneous maximum pressure head rise $(\Delta H)$ is governed by Joukowsky’s Equation: $\Delta H = \frac{a \cdot \Delta v}{g}$ Where $\Delta v$ is change in flow velocity and a is acoustic wave celerity through the fluid conduit $(a = \sqrt{\frac{K/\rho}{1 + \frac{K \cdot D}{E \cdot e}}}).$ Here, $K$ is fluid bulk modulus, $\rho$ is density, $D$ is pipe diameter, $E$ is wall modulus of elasticity, and $e$ is pipe wall thickness. To absorb high-pressure shock waves, Surge Tanks are installed upstream of penstocks. The maximum vertical surge height $(z_{max})$ in a simple surge tank of area $A_s$ following sudden total valve shutoff is: $z_{max} = v_0 \cdot \sqrt{\frac{A_p \cdot L}{g \cdot A_s}}$ Where $v_0$ is initial velocity, $A_p$ is penstock area, and L is conduit length. High-head hydroelectric plants in the steep valleys ...