Maximum Floating Needle Diameter Calculation

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Homework Help Overview

The discussion revolves around the calculation of the maximum diameter of a wax-coated stainless steel needle that can float on water, focusing on the principles of surface tension and buoyancy. The original poster has provided the surface tension value and the density of the needle, seeking guidance on how to approach the problem.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the weight of the needle and its relationship to surface tension, exploring various equations related to buoyancy and surface tension. There are attempts to derive the radius and diameter of the needle, with some questioning the correctness of their approaches and calculations.

Discussion Status

Several participants have provided insights and corrections to each other's reasoning, indicating a collaborative effort to clarify the problem. There is an ongoing exploration of different methods to calculate the maximum diameter, with some participants suggesting that the weight may not be necessary for the final calculation.

Contextual Notes

Participants are working under the assumption that the needle is cylindrical and are considering the effects of surface tension and density in their calculations. There is some uncertainty regarding the application of certain formulas and the relevance of ambient pressure in this context.

hcho88
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Homework Statement


First part of the question was "Why is it possible to float a wax-coated stainless steel needle on the surface of water?" and I've already answered that, but I'm having trouble with the second part of the question, which is:

If the surface tension at the interface is 0.073 N/m and the density of the steel needle is 7.8x10^3 kg/m^3, what is the maximum diameter of a needle that can float this way? (Hint: start by finding the weight of the needle. You may assume that the needle is cylindrical in cross-section)


Homework Equations


Density = mass / volume
h = (2[tex]\sigma[/tex]cos[tex]\Psi[/tex]) / ([tex]\rho[/tex]g[tex]\alpha[/tex])
V of needle = width x (2[tex]\Pi[/tex]r^2)
I'm actually not too sure which equations I need...



The Attempt at a Solution


[tex]\sigma[/tex] = 0.073N/m
[tex]\rho[/tex] of stainless steel needle = 7.8x10^3 kg/m^3
Well it says to start by finding the weight of the needle, and I wasn't sure how to approach that in the first place, so I wasn't able to make a start.
 
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hikaru1221 said:
Have a look at this site: http://en.wikipedia.org/wiki/Surface_tension#Basic_physics See the first picture and you may know what's next to do :wink:

[tex]\Sigma[/tex]F = 0
-W + ([tex]\sigma[/tex]L)cos[tex]\vartheta[/tex] + ([tex]\sigma[/tex]L)cos[tex]\vartheta[/tex] = 0
W = 2([tex]\sigma[/tex]L)cos[tex]\vartheta[/tex]
W = 2 x 0.073 x L x 1
W = 0.146L N

Is this correct?
I have absolutely no idea what to do next.
Just guessing, please correct me if I'm wrong...
Mass of needle = 0.146L/9.8 kg
Volume of needle = ([tex]\Pi[/tex]r^2)*L
Volume of needle = 1/([tex]\rho[/tex]m) = 1/(7.8x10^3 x 0.015L) = 8.61x10^-3L m^3
So 8.61x10^-3L = ([tex]\Pi[/tex]r^2)*L
8.61x10^-3 = [tex]\Pi[/tex]r^2
r = 0.05 m

I've found a radius of some sort, but I don't think it's right.
The question says I need to find the maximum diameter of a needle that can float.
How do I find this?
 
Last edited:
Hold on...
I have another theory! Please tell me which one is wrong or right or both are wrong! :S
[tex]\Sigma[/tex]F = 0
-W + ([tex]\sigma[/tex]Lcos[tex]\theta[/tex]) + ([tex]\sigma[/tex]Lcos[tex]\theta[/tex]) = 0
W = 2([tex]\sigma[/tex]L)cos[tex]\theta[/tex]
W = 2 x 0.073 x L x 1
W = 0.146L N

And using another formula:
P = (2[tex]\sigma[/tex]) / r
P = 101325 Pa
So, r = (2 x 0.073) / 101325
r = 1.44x10^-6 m

Or is this formula only used for bubbles?

anyway, my other answer to this problem being
d=2r
d=2.88x10^-6m

Please tell me where I went wrong and how I should tackle this problem to solve it.
Please give me directions!
Thank you!
 
[tex]8.61\times 10^-3L = \pi r^2L[/tex]
You have gone this far and there is just one more minor step to the result :wink: L is canceled as it appears in both sides, so there is only 1 unknown left :biggrin: By the way, please check your numerical values, because I'm too lazy to check them :biggrin:

P = (2LaTeX Code: \\sigma ) / r
P = 101325 Pa
So, r = (2 x 0.073) / 101325
r = 1.44x10^-6 m
So there is no need for the weight, right?
The effect is due to surface tension, not ambient pressure.

EDIT: I've just read again your post and found you made some corrections. You were on the right track at post #3. Now I'll organize it a bit:
[tex]W=2\sigma Lcos\theta[/tex]
[tex]\rho g \pi r^2L=2\sigma Lcos\theta[/tex]
[tex]r=\sqrt{\frac{2\sigma cos\theta}{\rho g \pi}}[/tex]
As you can see, r is max when cos(theta) is max, and max of cos(theta) is 1. You will find that [tex]r_{max} = 0.78mm[/tex], not so large as 0.05m that you got earlier.
 
Last edited:
Thank you
 

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