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Hydraulic Jump01:29

Hydraulic Jump

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A hydraulic jump is a sudden rise in fluid depth in open channels, occurring when high-velocity (supercritical) flow transitions to low-velocity (subcritical) flow. This phenomenon requires an upstream Froude number greater than 1, as flows with Fr1<1 remain subcritical, making a hydraulic jump impossible due to the need for negative head loss, which violates thermodynamic principles.The characteristics of a hydraulic jump depend on the upstream Froude number and are classified as...
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Hydraulic Jump: Problem Solving01:16

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To analyze a hydraulic jump in a rectangular channel with a flow speed of 6 meters per second, follow these steps:Calculate Effective Upstream Velocity:When the downstream gate closes, a hydraulic jump forms, traveling upstream at 2 meters per second. This wave speed combines with the initial channel flow velocity, creating an effective upstream velocity.Identify Flow Velocities Before and After the Hydraulic Jump:Upstream of the hydraulic jump, the effective flow velocity includes both the...
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Precipitation Processes01:12

Precipitation Processes

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The experimental conditions in a gravimetric analysis should be optimized to maximize the particle size and purity of the obtained precipitate. Ideally, the concentration of the precipitating reagent should be low with effective stirring to maintain low relative supersaturation for the growth of large crystals. In homogeneous precipitation, the precipitant is slowly generated by a chemical reaction in the solution to avoid local reagent excesses. For example, urea decomposes gradually to...
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Excess Pressure Inside a Drop and a Bubble01:13

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The shape of a small drop of liquid can be considered spherical, neglecting the effect of gravity. This drop can further be considered as two equal hemispherical drops put together due to surface tension. The forces acting on the spherical drop are due to the pressure of the liquid inside the drop, the pressure due to air outside the drop, and the force due to the surface tension acting on the two hemispherical drops.
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Shock Waves01:16

Shock Waves

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While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...
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Design Example: Creating a Hydraulic Model of a Dam Spillway01:21

Design Example: Creating a Hydraulic Model of a Dam Spillway

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Scaled hydraulic models of dam spillways provide a practical way to replicate and study the intricate flow dynamics of these structures. Often built to a 1:15 ratio, these models allow for observing critical water behavior, such as velocity distribution, flow patterns, and energy dissipation.
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Updated: Oct 20, 2025

Visualization of High Speed Liquid Jet Impaction on a Moving Surface
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Hydraulic jump dynamics above supercell thunderstorms.

Morgan E O'Neill1, Leigh Orf2,3, Gerald M Heymsfield3,4

  • 1Department of Earth System Science, Stanford University, Stanford, CA 94305, USA.

Science (New York, N.Y.)
|September 13, 2021
PubMed
Summary
This summary is machine-generated.

Strongest thunderstorms create above-anvil cirrus plumes (AACP) by acting like mountains, injecting significant water vapor into the stratosphere. This process impacts ozone and climate.

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Area of Science:

  • Atmospheric Science
  • Meteorology
  • Climate Science

Background:

  • Above-anvil cirrus plumes (AACP) are linked to strong supercell thunderstorms.
  • The stratospheric hydration from AACP has an unclear role in ozone depletion and global warming.
  • Understanding AACP formation is crucial for climate modeling.

Purpose of the Study:

  • To investigate the physical mechanisms behind above-anvil cirrus plume generation.
  • To quantify the potential for stratospheric water vapor injection by supercells.

Main Methods:

  • Utilized large eddy simulations to model AACP formation.
  • Corroborated simulation results with radar observations.
  • Analyzed the interaction between overshooting convection and stratospheric flow.

Main Results:

  • The overshooting top of a supercell acts as a topographic obstacle.
  • A hydraulic jump forms at the tropopause, analogous to mountain-induced windstorms.
  • Simulated water vapor injection into the stratosphere can exceed 7 tonnes per second.

Conclusions:

  • The study elucidates the mechanism of AACP generation via a tropopause hydraulic jump.
  • Supercell thunderstorms can significantly hydrate the lower stratosphere.
  • Findings highlight a key process impacting stratospheric chemistry and climate.