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Draft Tube Flow. u 1. c 1. w 1. u 2. w 2. c 2. Swirl at the outlet from Francis runners. u 2. b 2. c 2. w 2. c 2u. u 2. b 2. c 2. c 2m. w 2. c 2u. u 2. b 2. c 2m. w 2. c 2. Phenomenon in the draft tube flow Swirl flow Flow in bend
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u1 c1 w1 u2 w2 c2 Swirl at the outlet from Francis runners u2 b2 c2 w2 c2u u2 b2 c2 c2m w2 c2u u2 b2 c2m w2 c2
Phenomenon in the draft tube flow • Swirl flow • Flow in bend • Positive pressure gradient in the diffuser - separation
Swirl flow in draft tubes • Strong coupling between the flow field and the pressure gradients Anisotropic turbulence • The turbulence is influenced by the geometry and the velocity • The draft tube flow is sensitive to the inlet conditions (velocity and pressure) • A vortex filament is present
Mean Axial Velocity Swirl flow
Vortex breakdown Vortex breakdown is present when a negative axial velocity occurs in the center of the flow. Vortex breakdown occurs when S > 1
Rankine Vortex Swirl flow
Swirl flow Vortex filament at part load Vortex filament at full load
Flow in bends A - A A A
Flow in bends Newton’s 2 law From Bernoulli’s equation Free Vortex
Results: The hydraulic design of the draft tube gives secondary flow and therefore a reduced efficiency
The Navier Stokes equations in Cylindrical coordinates r-direction: q-direction: z-direction:
Euler equations r-direction: q-direction: z-direction:
r-direction • Assume steady state solution • Assume axis symmetry • Assume g-force to be neglectible
0,1 m Pressure [Pa]
0,1 m Pressure [Pa] Radius [m]
0,2 m Pressure [Pa]
0,2 m Pressure [Pa] Radius [m]
0,4 m Pressure [Pa]
0,4 m Pressure [Pa] Radius [m]