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Babaria Institute Of
Technology, Vadodara.
Applied Fluid Mechenics.
A Presentation on
‘Rapidly Variying Flow’
By:-
Milan Sheta(130050106109)
Vikram Sindhav(130050106111)
Introduction
• Rapidly-varied flow is a significant change in
water depth over a short distance (a few times
water depth).
• It occurs where there is a local disturbance to
the balance between gravity and friction (e.g.
at a weir, venturi, sluice, free overfall, sudden
change in slope, ...) or a mismatch between
the depths imposed by upstream and
downstream conditions (hydraulic jump).
• Often there is a critical flow transition
between deep, slow flow (subcritical; Fr < 1)
and shallow, fast flow (supercritical; Fr > 1).
• The assumption that the flow varies rapidly
over a relatively short distance means that
bed friction is unimportant. Thus, for a
smooth transition (e.g. weir, venturi or sluice),
the total head is usually assumed constant
through this short region.
• For an abrupt transition (hydraulic jump) there
may be significant head loss, but it is
associated with high levels of turbulence, not
bed friction.
• Note that the hydrostatic pressure assumption
can only be applied where near-parallel flow
has been re-established, either side of the
rapidly-varying-flow region.
Hydraulic Jump
• A hydraulic jump is an abrupt change from a
shallow, high-speed flow to a deep, low-speed
flow of lower energy.
• It occurs when a depth difference is imposed
by upstream and downstream conditions.
Rapid, shallow flow may be created by, for
example, a steep spillway or sluice.
• A slower and deeper downstream flow may be
controlled by a downstream weir or by a
reduction in slope.
• The triggering of a hydraulic jump at the base
of a spillway is desirable to remove surplus
kinetic energy in order to reduce downstream
erosion.
V1
h2
h1
V2
Across a hydraulic jump
• Mass is conserved.
• The momentum principle is satisfied.
• Mechanical energy is lost (mostly as heat).
Assume, for simplicity
• Small slope (downslope component of weight
of can be neglected).
• Wide or rectangular cross-section.
• Velocity uniform over upstream and
downstream cross-sections.
• The length of the jump is short (so that bed
friction can be neglected).
Thank You

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Rapidly variying flow

  • 1. Babaria Institute Of Technology, Vadodara. Applied Fluid Mechenics. A Presentation on ‘Rapidly Variying Flow’ By:- Milan Sheta(130050106109) Vikram Sindhav(130050106111)
  • 2. Introduction • Rapidly-varied flow is a significant change in water depth over a short distance (a few times water depth). • It occurs where there is a local disturbance to the balance between gravity and friction (e.g. at a weir, venturi, sluice, free overfall, sudden change in slope, ...) or a mismatch between the depths imposed by upstream and downstream conditions (hydraulic jump).
  • 3. • Often there is a critical flow transition between deep, slow flow (subcritical; Fr < 1) and shallow, fast flow (supercritical; Fr > 1). • The assumption that the flow varies rapidly over a relatively short distance means that bed friction is unimportant. Thus, for a smooth transition (e.g. weir, venturi or sluice), the total head is usually assumed constant through this short region.
  • 4. • For an abrupt transition (hydraulic jump) there may be significant head loss, but it is associated with high levels of turbulence, not bed friction. • Note that the hydrostatic pressure assumption can only be applied where near-parallel flow has been re-established, either side of the rapidly-varying-flow region.
  • 5. Hydraulic Jump • A hydraulic jump is an abrupt change from a shallow, high-speed flow to a deep, low-speed flow of lower energy. • It occurs when a depth difference is imposed by upstream and downstream conditions. Rapid, shallow flow may be created by, for example, a steep spillway or sluice. • A slower and deeper downstream flow may be controlled by a downstream weir or by a reduction in slope.
  • 6. • The triggering of a hydraulic jump at the base of a spillway is desirable to remove surplus kinetic energy in order to reduce downstream erosion. V1 h2 h1 V2
  • 7.
  • 8.
  • 9. Across a hydraulic jump • Mass is conserved. • The momentum principle is satisfied. • Mechanical energy is lost (mostly as heat).
  • 10. Assume, for simplicity • Small slope (downslope component of weight of can be neglected). • Wide or rectangular cross-section. • Velocity uniform over upstream and downstream cross-sections.
  • 11. • The length of the jump is short (so that bed friction can be neglected).