fluid_mechanics
290 Chapter 6 ■ Differential Analysis of Fluid Flow SOLUTION The components of velocity are v r 0f 0r 2 r which indicates we have a purely radial flow. The flowrate per unit width, q, crossing the arc of length Rp6 can thus be obtained by integrating the expression COMMENT Note that the radius R is arbitrary since the v u 1 flowrate crossing any curve between the two walls must be the 0f r 0u 0 same. The negative sign indicates that the flow is toward the opening, that is, in the negative radial direction. p6 p6 q v r R du a 2 R b R du 0 0 p 3 1.05 ft2 s (Ans) 6.5.3 Vortex We next consider a flow field in which the streamlines are concentric circles—that is, we interchange the velocity potential and stream function for the source. Thus, let f Ku (6.84) A vortex represents a flow in which the streamlines are concentric circles. and (6.85) where K is a constant. In this case the streamlines are concentric circles as are illustrated in Fig. 6.18, with v r 0 and v u 1 r c K ln r 0f 0u 0c 0r K r (6.86) v θ v θ ~ 1__ r r This result indicates that the tangential velocity varies inversely with the distance from the origin, as shown by the figure in the margin, with a singularity occurring at r 0 1where the velocity becomes infinite2. It may seem strange that this vortex motion is irrotational 1and it is since the flow field is described by a velocity potential2. However, it must be recalled that rotation refers to the orientation of a fluid element and not the path followed by the element. Thus, for an irrotational vortex, if a pair of small sticks were placed in the flow field at location A, as indicated in Fig. 6.19a, the sticks would rotate as they move to location B. One of the sticks, the one that is aligned along the streamline, would follow a circular path and rotate in a counterclockwise y ψ = constant v θ r θ x φ = constant F I G U R E 6.18 pattern for a vortex. The streamline
6.5 Some Basic, Plane Potential Flows 291 B A v 1_ θ ~ r B A v ~ r θ r r (a) (b) F I G U R E 6.19 Motion of fluid element from A to B: (a) for irrotational (free) vortex; (b) for rotational (forced) vortex. Vortex motion can be either rotational or irrotational. direction. The other stick would rotate in a clockwise direction due to the nature of the flow field—that is, the part of the stick nearest the origin moves faster than the opposite end. Although both sticks are rotating, the average angular velocity of the two sticks is zero since the flow is irrotational. If the fluid were rotating as a rigid body, such that v u K 1 r where K 1 is a constant, then sticks similarly placed in the flow field would rotate as is illustrated in Fig. 6.19b. This type of vortex motion is rotational and cannot be described with a velocity potential. The rotational vortex is commonly called a forced vortex, whereas the irrotational vortex is usually called a free vortex. The swirling motion of the water as it drains from a bathtub is similar to that of a free vortex, whereas the motion of a liquid contained in a tank that is rotated about its axis with angular velocity v corresponds to a forced vortex. A combined vortex is one with a forced vortex as a central core and a velocity distribution corresponding to that of a free vortex outside the core. Thus, for a combined vortex v u vr r r 0 (6.87) and v u K r r 7 r 0 (6.88) where K and v are constants and r 0 corresponds to the radius of the central core. The pressure distribution in both the free and forced vortex was previously considered in Example 3.3. (See Fig. E6.6a for an approximation of this type of flow.) F l u i d s i n t h e N e w s Some hurricane facts One of the most interesting, yet potentially devastating, naturally occurring fluid flow phenomenan is a hurricane. Broadly speaking a hurricane is a rotating mass of air circulating around a low pressure central core. In some respects the motion is similar to that of a free vortex. The Caribbean and Gulf of Mexico experience the most hurricanes, with the official hurricane season being from June 1 to November 30. Hurricanes are usually 300 to 400 miles wide and are structured around a central eye in which the air is relatively calm. The eye is surrounded by an eye wall which is the region of strongest winds and precipitation. As one goes from the eye wall to the eye the wind speeds decrease sharply and within the eye the air is relatively calm and clear of clouds. However, in the eye the pressure is at a minimum and may be 10% less than standard atmospheric pressure. This low pressure creates strong downdrafts of dry air from above. Hurricanes are classified into five categories based on their wind speeds: Category one—74–95 mph Category two—96–110 mph Category three—111–130 mph Category four—131–155 mph Category five—greater than 155 mph. (See Problem 6.58.)
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6.5 Some Basic, Plane Potential Flows 291<br />
B<br />
A<br />
v<br />
1_ θ ~ r<br />
B<br />
A<br />
v ~ r<br />
θ<br />
r<br />
r<br />
(a)<br />
(b)<br />
F I G U R E 6.19 Motion of <strong>fluid</strong> element from A to B: (a) for<br />
irrotational (free) vortex; (b) for rotational (forced) vortex.<br />
Vortex motion can<br />
be either rotational<br />
or irrotational.<br />
direction. The other stick would rotate in a clockwise direction due to the nature of the flow<br />
field—that is, the part of the stick nearest the origin moves faster than the opposite end. Although<br />
both sticks are rotating, the average angular velocity of the two sticks is zero since the flow is<br />
irrotational.<br />
If the <strong>fluid</strong> were rotating as a rigid body, such that v u K 1 r where K 1 is a constant, then<br />
sticks similarly placed in the flow field would rotate as is illustrated in Fig. 6.19b. This type of<br />
vortex motion is rotational and cannot be described with a velocity potential. The rotational vortex<br />
is commonly called a forced vortex, whereas the irrotational vortex is usually called a free vortex.<br />
The swirling motion of the water as it drains from a bathtub is similar to that of a free vortex,<br />
whereas the motion of a liquid contained in a tank that is rotated about its axis with angular velocity<br />
v corresponds to a forced vortex.<br />
A combined vortex is one with a forced vortex as a central core and a velocity distribution<br />
corresponding to that of a free vortex outside the core. Thus, for a combined vortex<br />
v u vr r r 0<br />
(6.87)<br />
and<br />
v u K r<br />
r 7 r 0<br />
(6.88)<br />
where K and v are constants and r 0 corresponds to the radius of the central core. The pressure<br />
distribution in both the free and forced vortex was previously considered in Example 3.3. (See Fig.<br />
E6.6a for an approximation of this type of flow.)<br />
F l u i d s i n t h e N e w s<br />
Some hurricane facts One of the most interesting, yet potentially<br />
devastating, naturally occurring <strong>fluid</strong> flow phenomenan is a hurricane.<br />
Broadly speaking a hurricane is a rotating mass of air circulating<br />
around a low pressure central core. In some respects the motion<br />
is similar to that of a free vortex. The Caribbean and Gulf of Mexico<br />
experience the most hurricanes, with the official hurricane season<br />
being from June 1 to November 30. Hurricanes are usually 300 to<br />
400 miles wide and are structured around a central eye in which<br />
the air is relatively calm. The eye is surrounded by an eye wall<br />
which is the region of strongest winds and precipitation. As one<br />
goes from the eye wall to the eye the wind speeds decrease sharply<br />
and within the eye the air is relatively calm and clear of clouds.<br />
However, in the eye the pressure is at a minimum and may be 10%<br />
less than standard atmospheric pressure. This low pressure creates<br />
strong downdrafts of dry air from above. Hurricanes are classified<br />
into five categories based on their wind speeds:<br />
Category one—74–95 mph<br />
Category two—96–110 mph<br />
Category three—111–130 mph<br />
Category four—131–155 mph<br />
Category five—greater than 155 mph.<br />
(See Problem 6.58.)