Question 8..8: Under what conditions can you compute the pressure in the sy...

Under what conditions can you compute the pressure in the system in Fig. 8.15? Recall that streamlines must be parallel and straight, where the radius of curvature is infinity, in order for \partial p/\partial n=0. Consider multiple possibilities.

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For flow along a streamline between points 2 and 4,

                             \frac{p_{2}}{\rho }+gz_{2}+\frac{1}{2}\nu ^{2}_{2}=\frac{p_{4}}{\rho }+gz_{4}+\frac{1}{2}\nu ^{2}_{4}.

From overall mass balance,   \nu _{2}A_{2}=\nu _{4}A_{4}. For the pipe from point 2 to point 4,  A_{2}=A_{4};  therefore,   \nu _{2}=\nu _{4}.   With \nu _{2}=\nu _{4} and z_{2}=z_{4}, Bernoulli’s equation FIGURE 8.15 Flow from a reservoir through a segment of rigid tubing. suggests that the pressures p_{2} and p_{4} are equal. Because we discharge to atmospheric pressure at an assumed subsonic velocity, p_{4}=0 (gauge) and the pressure at point 2 is also predicted to be zero. Would we expect this to be the case particularly given that we are driving the flow only via a pressure gradient? Recall that Bernoulli should not be used over long distances. For flow along a streamline between points 1 and 2, assuming a rounded entrance at the chamber-tube interface,

                                                         \frac{p_{1}}{\rho }+gz_{1}+\frac{1}{2}\nu ^{2}_{1}=\frac{p_{2}}{\rho }+gz_{2}+\frac{1}{2}\nu ^{2}_{2},

where the pressure at point 1 is zero (gauge) and v_{1}\ll \nu _{2}  if    A_{1}\gg A_{2}; thus,

                                             gz_{1}=\frac{p_{2}}{\rho }+\frac{1}{2}\nu ^{2}_{2}\rightarrow p_{2}=\rho gH-\frac{1}{2}\rho \nu ^{2}_{2},

where \nu _{2} is nonzero and equal to \nu _{3} (which is measured via the flowmeter) by mass balance. We observe, therefore, that one application of Bernoulli suggests that p_{2}=0, whereas another yields P_{2}=\rho gH-½\rho \nu ^{2}_{2}. Bernoulli is applicable across contractions and over short distances.

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