Froude number: Difference between revisions

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#<div class="definition"><div class="short_definition">The nondimensional ratio of the [[inertial force]] to the [[force of gravity]] for a  given fluid flow; the reciprocal of the [[Reech number]].</div><br/> <div class="paragraph">It may be given as  <div class="display-formula"><blockquote>[[File:ams2001glos-Fe21.gif|link=|center|ams2001glos-Fe21]]</blockquote></div> where ''V'' is a [[characteristic velocity]], ''L'' a [[characteristic length]], and ''g'' the [[acceleration of gravity]];  or as the square root of this number.</div><br/> </div>
#<div class="definition"><div class="short_definition">The nondimensional ratio of the [[inertial force]] to the [[force of gravity]] for a  given fluid flow; the reciprocal of the [[Reech number]].</div><br/> <div class="paragraph">It may be given as  <div class="display-formula"><blockquote>[[File:ams2001glos-Fe21.gif|link=|center|ams2001glos-Fe21]]</blockquote></div> where ''V'' is a [[characteristic velocity]], ''L'' a [[characteristic length]], and ''g'' the [[acceleration of gravity]];  or as the square root of this number.</div><br/> </div>
#<div class="definition"><div class="short_definition">For atmospheric flows over hills or other obstacles, a more useful form of the Froude number  is  <div class="display-formula"><blockquote>[[File:ams2001glos-Fe22.gif|link=|center|ams2001glos-Fe22]]</blockquote></div> where ''N''<sub>''BV''</sub> is the [[Brunt&ndash;V&#x000e4;is&#x000e4;l&#x000e4; frequency]] of the ambient [[upstream]] environment, ''V'' is the [[wind  speed]] component across the mountain, and ''L''<sub>''w''</sub> is the width of the mountain. </div><br/> <div class="paragraph">Fr can be interpreted as the ratio of natural [[wavelength]] of the air to wavelength of the mountain.  Sometimes &#x003c0; will appear in the numerator, and other times the ratio will be squared. When Fr =  1, the natural wavelength of the air is in [[resonance]] with the size of the mountain and creates the  most intense [[mountain waves]], which can sometimes contain [[lenticular clouds]] and [[rotors]] of  reverse flow at the surface. For Fr &lt; 1, some of the low-altitude upstream air is blocked by the  hill, short-wavelength waves separate from the top of the hill, and the remaining air at lower  altitudes flows laterally around the hill. For Fr &gt; 1, very long wavelengths form [[downwind]] of the  hill, and can include a [[cavity]] of reverse flow just to the lee of the hill near the surface. Another  form of the Froude number, using (''z''<sub>''i''</sub> - ''z''<sub>''hill''</sub>) in place of ''L''<sub>''w''</sub>, is useful for diagnosing downslope  windstorms and [[hydraulic jump]], where ''z''<sub>''i''</sub> is the depth of the [[mixed layer]] above the base of the  mountain, and ''z''<sub>''hill''</sub> is the height of the mountain.</div><br/> </div>
#<div class="definition"><div class="short_definition">For atmospheric flows over hills or other obstacles, a more useful form of the Froude number  is  <div class="display-formula"><blockquote>[[File:ams2001glos-Fe22.gif|link=|center|ams2001glos-Fe22]]</blockquote></div> where ''N''<sub>''BV''</sub> is the [[Brunt&ndash;V&#x000e4;is&#x000e4;l&#x000e4; frequency]] of the ambient [[upstream]] environment, ''V'' is the [[wind speed|wind  speed]] component across the mountain, and ''L''<sub>''w''</sub> is the width of the mountain. </div><br/> <div class="paragraph">Fr can be interpreted as the ratio of natural [[wavelength]] of the air to wavelength of the mountain.  Sometimes &#x003c0; will appear in the numerator, and other times the ratio will be squared. When Fr =  1, the natural wavelength of the air is in [[resonance]] with the size of the mountain and creates the  most intense [[mountain waves]], which can sometimes contain [[lenticular clouds]] and [[rotors]] of  reverse flow at the surface. For Fr &lt; 1, some of the low-altitude upstream air is blocked by the  hill, short-wavelength waves separate from the top of the hill, and the remaining air at lower  altitudes flows laterally around the hill. For Fr &gt; 1, very long wavelengths form [[downwind]] of the  hill, and can include a [[cavity]] of reverse flow just to the lee of the hill near the surface. Another  form of the Froude number, using (''z''<sub>''i''</sub> - ''z''<sub>''hill''</sub>) in place of ''L''<sub>''w''</sub>, is useful for diagnosing downslope  windstorms and [[hydraulic jump]], where ''z''<sub>''i''</sub> is the depth of the [[mixed layer]] above the base of the  mountain, and ''z''<sub>''hill''</sub> is the height of the mountain.</div><br/> </div>
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Revision as of 16:02, 25 April 2012



Froude number[edit | edit source]

  1. The nondimensional ratio of the inertial force to the force of gravity for a given fluid flow; the reciprocal of the Reech number.

    It may be given as
    ams2001glos-Fe21
    where V is a characteristic velocity, L a characteristic length, and g the acceleration of gravity; or as the square root of this number.

  2. For atmospheric flows over hills or other obstacles, a more useful form of the Froude number is
    ams2001glos-Fe22
    where NBV is the Brunt–Väisälä frequency of the ambient upstream environment, V is the wind speed component across the mountain, and Lw is the width of the mountain.

    Fr can be interpreted as the ratio of natural wavelength of the air to wavelength of the mountain. Sometimes π will appear in the numerator, and other times the ratio will be squared. When Fr = 1, the natural wavelength of the air is in resonance with the size of the mountain and creates the most intense mountain waves, which can sometimes contain lenticular clouds and rotors of reverse flow at the surface. For Fr < 1, some of the low-altitude upstream air is blocked by the hill, short-wavelength waves separate from the top of the hill, and the remaining air at lower altitudes flows laterally around the hill. For Fr > 1, very long wavelengths form downwind of the hill, and can include a cavity of reverse flow just to the lee of the hill near the surface. Another form of the Froude number, using (zi - zhill) in place of Lw, is useful for diagnosing downslope windstorms and hydraulic jump, where zi is the depth of the mixed layer above the base of the mountain, and zhill is the height of the mountain.


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