3. Figure shows a stream of water flowing through a circular hole at depth y. The diameters of the cylindrical container and the hole are √2D and D, respectively. We define v and V by the speeds of the water flow on the water surface and that at the hole, respectively. We assume that the water is an ideal fluid. The density of water is p and the gravitational acceleration is g. The atmospheric pressure is po everywhere in the laboratory. √2D Ро す A y υν V B (5) Let T be the time for draining water completely from the initial level y = yo to y = 0. Evaluate T in terms of g and yo. (6) Let M be the mass of the water initially contained in the tank with y = yo. Let K be the sum of the kinetic energy of the water flowing out of the hole from t = 0 to T. Evaluate K in terms of M, g, and Yo.
3. Figure shows a stream of water flowing through a circular hole at depth y. The diameters of the cylindrical container and the hole are √2D and D, respectively. We define v and V by the speeds of the water flow on the water surface and that at the hole, respectively. We assume that the water is an ideal fluid. The density of water is p and the gravitational acceleration is g. The atmospheric pressure is po everywhere in the laboratory. √2D Ро す A y υν V B (5) Let T be the time for draining water completely from the initial level y = yo to y = 0. Evaluate T in terms of g and yo. (6) Let M be the mass of the water initially contained in the tank with y = yo. Let K be the sum of the kinetic energy of the water flowing out of the hole from t = 0 to T. Evaluate K in terms of M, g, and Yo.
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![3. Figure shows a stream of water flowing through a circular hole at depth y. The diameters
of the cylindrical container and the hole are √2D and D, respectively. We define v and
V by the speeds of the water flow on the water surface and that at the hole, respectively.
We assume that the water is an ideal fluid. The density of water is p and the gravitational
acceleration is g. The atmospheric pressure is po everywhere in the laboratory.
√2D
Ро
す
A
y
υν
V
B
(5) Let T be the time for draining water completely from the initial level y = yo to y = 0.
Evaluate T in terms of g and yo.
(6) Let M be the mass of the water initially contained in the tank with y = yo. Let K be
the sum of the kinetic energy of the water flowing out of the hole from t = 0 to T. Evaluate
K in terms of M, g, and Yo.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F70454126-824a-4305-adda-0040decf2e01%2F51bf193b-a60d-4a64-bfde-79a1089b5c6d%2Fkqcrf7n_processed.jpeg&w=3840&q=75)
Transcribed Image Text:3. Figure shows a stream of water flowing through a circular hole at depth y. The diameters
of the cylindrical container and the hole are √2D and D, respectively. We define v and
V by the speeds of the water flow on the water surface and that at the hole, respectively.
We assume that the water is an ideal fluid. The density of water is p and the gravitational
acceleration is g. The atmospheric pressure is po everywhere in the laboratory.
√2D
Ро
す
A
y
υν
V
B
(5) Let T be the time for draining water completely from the initial level y = yo to y = 0.
Evaluate T in terms of g and yo.
(6) Let M be the mass of the water initially contained in the tank with y = yo. Let K be
the sum of the kinetic energy of the water flowing out of the hole from t = 0 to T. Evaluate
K in terms of M, g, and Yo.
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