Fluid mechanics mercury problem

Click For Summary
SUMMARY

The forum discussion centers on solving 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 10.0 cm², while the right arm has an area of 5.00 cm². The user successfully calculated the height of the water column in the right arm as 20 cm but struggled with determining the height of mercury rise in the left arm. The correct approach involves applying the principle of hydrostatic equilibrium and equating the volumes of fluid displaced, leading to a final mercury rise of 0.49 cm.

PREREQUISITES
  • Understanding of hydrostatic pressure and equilibrium
  • Knowledge of fluid density calculations
  • Familiarity with the concept of volume displacement in fluids
  • Basic algebra for solving equations
NEXT STEPS
  • Study the principles of hydrostatic equilibrium in fluid mechanics
  • Learn about fluid density and its role in buoyancy
  • Explore volume displacement calculations in U-tube problems
  • Practice solving similar fluid mechanics problems using different fluids
USEFUL FOR

Students studying fluid mechanics, educators teaching physics concepts, and anyone interested in understanding hydrostatic principles and U-tube applications.

clairez93
Messages
113
Reaction score
0

Homework Statement



Mercury is poured into a U-tube as in Figure P15.18a. [see the picture here: http://www.ux1.eiu.edu/~cfadd/1350/Hmwk/Ch15/Images/P15.18.gif] The left arm of the tube has a cross-sectional area of A1 = 10.0 cm2, and the right arm has a cross-sectional area of A2 = 5.00 cm2. One hundred grams of water are then poured into the right arm as in Figure P15.18b.

(a) Determine the length of the water column in the right arm of the U-tube.

(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



\rho*gh_{i} = \rho*gh_{f} (at same level)
\rho = \frac{m}{v}


The Attempt at a Solution



I figured out a):
V = Ah
\rho = \frac{m}{v}
\rho = \frac{m}{Ah}
1000 = \frac{0.1}{(5*10^{-4}*h}
h = 0.2 m = 20 cm

I couldn't do part b), so I finally went to Google the problem and found a solution on this website: http://www.ux1.eiu.edu/~cfadd/1350/Hmwk/Ch15/Ch15.html

Their solution says this:

\rho*gl_{1} = \rho*gl_{2}
This equation is taken at the point where the water on the right hand side meets the mercury as shown in the picture on the site. 1s is the distance from the top of the mercury on the left hand side to this point and l2 is the distance from the top of the water to that point.
(13.6)(9.8)(l_{1}) = (1)(20)(9.8)
l_{1} = 1.47 cm

I understand this part. This is the part of the solution I do not understand:

A_{1}h = A_{2}(1.47 - h)
10h = 5(1.47 - h)
h = 0.49 cm

Basically I don't understand why you would know to set the two volumes equal to each other? How do you know the volumes are the same?
 
Last edited by a moderator:
Physics news on Phys.org
The water on one side must have the same weight or mass as the Mercury on the other side (above the bottom of the water in both cases).
mass on left = mass on right
pV = 100 g
pAh = 100 g
solve for h. Looks like a little more than 0.7 cm.
 

Similar threads

  • · Replies 6 ·
Replies
6
Views
799
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 18 ·
Replies
18
Views
7K
  • · Replies 6 ·
Replies
6
Views
2K
Replies
4
Views
4K
Replies
10
Views
4K
Replies
7
Views
16K
  • · Replies 3 ·
Replies
3
Views
4K
  • · Replies 21 ·
Replies
21
Views
4K