Surface Tenstion in Water (Needle resting on water)

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Homework Help Overview

The discussion revolves around the concept of surface tension in water and its ability to support a needle. The original poster presents a problem involving a steel needle with a specified diameter, density, and surface tension, seeking to demonstrate the feasibility of this phenomenon and to determine the largest diameter needle that could be supported by surface tension.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the relationship between surface tension, mass, and the dimensions of the needle. There are attempts to derive equations relating these variables, with some questioning the role of the needle's length in the calculations. Others express confusion about the implications of their calculations and whether the equations used are appropriate for the scenario.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some have provided insights into the relationships between the forces involved, while others are grappling with the calculations and the assumptions made regarding the needle's dimensions and properties.

Contextual Notes

There is uncertainty regarding the correct interpretation of the length variable in the equations, and participants are navigating the implications of the density of steel in their calculations. The problem is structured as a two-part question, which may influence how participants approach the solution.

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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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