How to Calculate Capillary Rise on the ISS

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SUMMARY

The discussion focuses on calculating the capillary rise of water in a cylindrical capillary tube aboard the International Space Station (ISS). The parameters include a capillary length of 10 cm, an inner diameter of 500 µm, and a contact angle of approximately 0 degrees. The primary equation used is h = 2Tcos(θ)/(ρg), where T is the surface tension, ρ is the density of water, and g is the gravitational acceleration. The final calculated height of water rise is 6.5 cm, assuming a reduced gravity of 0.9 g, although the actual gravity on the ISS is effectively zero due to free fall conditions.

PREREQUISITES
  • Understanding of capillary action and related physics principles
  • Familiarity with fluid dynamics equations, specifically h = 2Tcos(θ)/(ρg)
  • Knowledge of the properties of water, including surface tension and density
  • Basic concepts of microgravity environments and their effects on fluid behavior
NEXT STEPS
  • Research the effects of microgravity on fluid dynamics in space environments
  • Explore the properties of capillary action in different fluids and materials
  • Learn about the design and function of experiments conducted on the ISS
  • Investigate the implications of fluid behavior in sealed environments, such as capillaries
USEFUL FOR

Students in physics or engineering, researchers studying fluid dynamics in microgravity, and professionals involved in designing experiments for space applications will benefit from this discussion.

yung_flower
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Homework Statement


Consider an experiment on the International Space Station, which is illustrated below. A cylindrical capillary of length L= 10. [cm] and inner diameter of dc=500. [µm] (sealed at one end), is positioned to contact a droplet of water, D = 1.0 [cm], which is floating in the ISS laboratory. Water is completely hydrophilic with the material of that capillary (contact angle is θ ≈ 0o). The temperature in the ISS laboratories is 20 [oC].

Question: How far the water will enter the capillary; i.e. determine ‘h’ as shown in the illustration
below

Homework Equations


I assume this is the most important equation for looking at it (but nothing is really given):
h=2Tcos(theta)/(prg)

All of these are also given:c=500 [µm]; R =250 [µm]; L= 0.1 [m]; µwater=0.001 [Pa s]; ρwater =1000 [kg/m3] ;
σwater-air =0.072 [N/m]; h = ? [m]

The Attempt at a Solution


Since we do not know gravity I tried to solve initially for Pint of the capillary

Pint=2T/R

Pint=576pa = 0.576kpa --> 0.00568 atm

(My assumption that pressure in ISS is that of Earth at sea level)
Po= 1 atm + 0.00568 atm = 1.00568 atm

Vcap= (L-dc/2)(pi)(dc/2)^2 + (2/3)pi(dc/2)^3
Vcap= 1.96 x 10^-5 L

nair=(1atm)(1.96 x 10^-5 L)/((0.08206 Latm/molK)(293K))
nair= 8.160 x 10^-7 mol

If that's the air in the capillary before capillary action, then the air will be compressed to the new pressure:
Po=1.00568 atm

Vair2= (8.160 x 10^-7 mol)(0.08206 Latm/mol K)(293 K)/1.00568 atm
Vair2= 1.951 x 10^-5 L = 1.951 x 10^-8 m^3

Vair2= (L-dc/2-h)pi(dc/2)^2 + (2/3)pi(dc/2)^3

height comes out to be:

h= 5.53 x 10^-4 m

That height seems way to small to be right

---------------------------------------------------

Then I thought maybe I could assume (using the internet) that gISS=gearth(0.9)

and use the equation:

h=2Tcos(theta)/(prg)

to get:

h=6.5 cm

^This answer makes a lot more sense to me but it doesn't feel like the right way to do the problem, seeing as we are not given the statement that the gravity on the ISS is 90% of that on earth. Am I missing something?

Thanks!

Screen Shot 2016-10-09 at 1.50.57 PM.png
 
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Hi yung_flower and welcome to PF. :welcome:

I think you may safely assume that the apparent g = 0 because the ISS that is in free fall. The equation that you quoted is derived by setting the capillary force equal to the weight of the column of liquid. Here you have no weight. What keeps the liquid from rising all the way up? Hint: The capillary is sealed at one end.
 

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