2017
DOI: 10.1088/1361-6552/aa8d21
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Liquid oscillations in a U-tube

Abstract: In hydrostatics, pressure measurement with U-gauges and their relationship to density is a well-known experiment. Very little is studied or experimented with the dynamics of the movement of a liquid in a U-tube probably due to its theoretical complexity but, after all, it is a simple damped oscillating system. In this paper we present a relatively simple experiment that allows studying in some detail the dynamics of the movement of a liquid in a U-tube when an initial pressure gradient is applied. In order to … Show more

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Cited by 3 publications
(6 citation statements)
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“…which is incorrect except at the instant when the free surfaces pass through the equilibrium level 4 so that y A = 0 = y B . (The pressure difference between points A and B is always zero, in contrast to what Hageseth claims [11][12][13].) Equation ( 1) reduces to the familiar formula for the variation in hydrostatic pressure with depth and so it should not be surprising that it does not apply to a dynamically oscillating liquid column.…”
Section: Analytic Solution For a U-tube Of Uniform Cross-sectional Areamentioning
confidence: 98%
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“…which is incorrect except at the instant when the free surfaces pass through the equilibrium level 4 so that y A = 0 = y B . (The pressure difference between points A and B is always zero, in contrast to what Hageseth claims [11][12][13].) Equation ( 1) reduces to the familiar formula for the variation in hydrostatic pressure with depth and so it should not be surprising that it does not apply to a dynamically oscillating liquid column.…”
Section: Analytic Solution For a U-tube Of Uniform Cross-sectional Areamentioning
confidence: 98%
“…According to equation(12), the acceleration of the fluid is zero at that instant and so the unsteady Bernoulli equation happens to reduce to equation (1) as the free surfaces pass through their equilibrium positions.…”
mentioning
confidence: 99%
“…A first approximation of the motion described by the fluid in a U-tube is given by considering only gravity and the so-called viscous frictional resistance between the fluid and the walls of the tube and neglecting the surface tension force at the upper surface of the liquid [13]. In this case, the total force on a small element of liquid ∆m is caused by the weight (see figure 1) and the damping term, parameterized by b, that can be described as proportional to the velocity 8 .…”
Section: Theoretical Descriptionmentioning
confidence: 99%
“…In this case, the total force on a small element of liquid ∆m is caused by the weight (see figure 1) and the damping term, parameterized by b, that can be described as proportional to the velocity 8 . The equation of motion can be written as follows [13] ρSL…”
Section: Theoretical Descriptionmentioning
confidence: 99%
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