Fluid mechanics - Pascal's principle

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SUMMARY

The discussion revolves around applying Pascal's principle to solve a fluid mechanics problem involving a U-tube filled with mercury and water. The left arm of the U-tube has a cross-sectional area of 9.4 cm², while the right arm has an area of 4.50 cm². The participant correctly identifies the equation P = P(o) + ρgh and formulates the relationship ρhggh = ρwghw to find the height of the mercury rise in the left arm after adding 100 grams of water to the right arm. The solution emphasizes the importance of equating head pressures on both sides of the tube, confirming the application of Pascal's law.

PREREQUISITES
  • Understanding of fluid mechanics principles, specifically Pascal's principle.
  • Familiarity with the equation P = P(o) + ρgh.
  • Knowledge of density calculations, particularly for mercury (13.6 g/cm³) and water.
  • Basic algebra skills for manipulating equations and solving for unknowns.
NEXT STEPS
  • Study the applications of Pascal's principle in various fluid systems.
  • Learn how to calculate pressure differences in U-tube manometers.
  • Explore the concept of hydrostatic pressure and its implications in fluid mechanics.
  • Investigate the effects of cross-sectional area on fluid height in connected tubes.
USEFUL FOR

Students studying fluid mechanics, physics educators, and anyone interested in understanding the principles of hydrostatics and fluid pressure systems.

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Homework Statement


Mercury is poured into a U-tube as shown in Figure a. The left arm of the tube has cross-sectional area A1 of 9.4 cm2, and the right arm has a cross-sectional area A2 of 4.50 cm2. One hundred grams of water are then poured into the right arm as shown in Figure b.
(b) Given that the density of mercury is 13.6 g/cm3, what distance h does the mercury rise in the left arm?

Homework Equations


P=P(o)+ρgh where ρ is density of subject in question

The Attempt at a Solution


Hey everyone, just need a little conceptual help here. I'm unsure how to find the height of the water and the reasoning behind it.
My equation is ρhggh = ρwghw
where hw is the height of water in the tube above the line. The volume displaced is equal, I'm that far but how does the water above the line factor into the calc? Or just set me straight for this, it seems the more I think about it the further I get from an answer, there's something I need to equate conceptually which I am not getting.
 

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Your equation is correct. Think about it this way: Using the original height of the mercury as the base line, the head pressure at that base line on the mercury side and the water side will be equal (a portion of Pascal's law).
 
thanks, worked through and got it
 

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