Surface Tenstion in Water (Needle resting on water)

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SUMMARY

The discussion centers on the physics of surface tension in water, specifically regarding the support of a needle by this force. Using the surface tension of water (0.072 N/m) and the density of steel (7900 kg/m³), participants calculated the maximum diameter of a needle that can be supported. The calculations indicate that a needle with a diameter of 0.25 mm can be supported, while the maximum diameter derived from the equations is approximately 1.54 mm. This discrepancy highlights the importance of accurately applying the equations of surface tension and mass.

PREREQUISITES
  • Understanding of surface tension and its formula (γ = F/L)
  • Knowledge of mass calculation using density (mass = density × volume)
  • Familiarity with the relationship between force, mass, and gravity (F = mg)
  • Basic algebra for manipulating equations and solving for variables
NEXT STEPS
  • Study the principles of surface tension in fluids and its applications
  • Learn about the effects of diameter on buoyancy and stability in liquids
  • Explore the derivation and application of the Young-Laplace equation
  • Investigate the role of material density in fluid mechanics
USEFUL FOR

Students in physics, particularly those studying fluid mechanics, engineers working with materials in liquid environments, and anyone interested in the practical applications of surface tension in everyday phenomena.

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Homework Statement


A needle can be supported by the suface tension of water.

Given the density of steel (7900kg/m^3) a needle with diameter 0.25mm, the surface tension of water (0.072 N/m) and acceleration due to gravity (9.8) show that this is reasonable.

What is the largest diameter needle that could be supported by the surface tension.

Homework Equations



<br /> \gamma=\frac{F}{L} \\<br /> \gamma L = mg \\<br /> 2 \gamma l = mg <br />
That last equation is for the largest possible mass

The Attempt at a Solution



So far I have done.
<br /> \gamma L = mg \\<br /> 0.072 × 2.5 × 10^{-4} = 9.8m \\<br /> 1.8×10^{-5}=9.8m<br />
But if I carry that through I get some crazy huge number for the mass which cannot be correct. I suspect that L is not the diameter of the needle but the true length but without that given I don't know how to find it. I know what to do or rather how to use all the values given apart from the density of steel so maybe that is relevant to my first issue but not sure how.
 
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The length affects both the surface tension force and the mass of the needle so the length should cancel...

Tension force = 2γ * length
Mass = density * area * length

So the force eqn is..

2γ * length = density * area * length * g

Length cancel.
 
CWatters said:
The length affects both the surface tension force and the mass of the needle so the length should cancel...

Tension force = 2γ * length
Mass = density * area * length

So the force eqn is..

2γ * length = density * area * length * g

Length cancel.

OK thanks. So is it always 2yL or only in the case when its the largest possible mass?
 
If I follow that through, I get confused, see if what I am doing is on the right path or not as its not working out (but I think it is not supposed to - I am not sure)

<br /> 2\gamma L=\rho ALg \\<br /> 2\gamma=\rho Ag \\<br /> 2×0.072=7900×g×A \\<br /> 0.144=77420A \\<br /> A=\frac{0.144}{77420}=1.86×10^{-6}<br /> \\<br /> \\<br /> A=\pi r^2 \\<br /> r=\sqrt{\frac{A}{\pi}}\\<br /> r=\sqrt{\frac{1.86×10^{-6}}{\pi}}=7.69× 10^{-4}m = 0.77mm<br />

And the diameter would be 1.54mm when it is only supposed to be 0.25mm.

I am really confused.
 
It looks like a two part question to me..

1) Show that surface tension can support a needle of diameter 0.25mm (eg show surface tension is greater than force due to gravity for that size).
2) Then calculate the maximum diameter that can be supported.
 

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