- #1
meldraft
- 281
- 2
Hey all,
I am designing a cup holder. It is supposed to be made out of a few steel rings. Its geometry is such that the hoops can open (so the radius increases), and you place the cup inside. Then, as the hoops spring back, they press upon the cup and the friction holds it in place as you lift the entire thing.
Making some rough assumptions (good accuracy is really not important at this point, I just want an order of magnitude), I thought I could use Laplace's Law for a cylindrical container, since my problem is basically the inverse (pressure is pointing inwards instead of outwards):
[tex]σ=\frac{PR}{t}[/tex]
where σ is the hoop tension, P the pressure of the hoop to the cup, r the radius of the ring, and t the ring's thickness. To simplify the problem a little, I can assume that my rings are infinitely thin (not in the radial direction where I do have thickness. in the z-direction.). Therefore, if N is the total normal force (and this is tricky, because the vector sum is 0):
[tex]P=\frac{N}{L}[/tex]
so P is a distributed force (Newton/m), much like a beam problem.
Now, since this is an elastic phenomenon, I used Hooke's Law, saying that:
[tex]εE=\frac{PR}{t}=\frac{NR}{Lt} => N=\frac{εELt}{R}[/tex]
Let traction be fmax:
[tex]fmax=μN[/tex]
By combining the last two equations:
[tex]fmax=\frac{μεELt}{R}[/tex]
I would have been perfectly fine with this result, but for strains above ε=10^-6, this formula yields outlandishly high values of friction. For instance, for ε=0.7, I would get something like 0.4 GigaNewtons. I probably went wrong somewhere, but I really can't locate the mistake! I would be grateful for any advice you can give me!
P.S. All calculations were done in SI, so this is after the units check :P
I am designing a cup holder. It is supposed to be made out of a few steel rings. Its geometry is such that the hoops can open (so the radius increases), and you place the cup inside. Then, as the hoops spring back, they press upon the cup and the friction holds it in place as you lift the entire thing.
Making some rough assumptions (good accuracy is really not important at this point, I just want an order of magnitude), I thought I could use Laplace's Law for a cylindrical container, since my problem is basically the inverse (pressure is pointing inwards instead of outwards):
[tex]σ=\frac{PR}{t}[/tex]
where σ is the hoop tension, P the pressure of the hoop to the cup, r the radius of the ring, and t the ring's thickness. To simplify the problem a little, I can assume that my rings are infinitely thin (not in the radial direction where I do have thickness. in the z-direction.). Therefore, if N is the total normal force (and this is tricky, because the vector sum is 0):
[tex]P=\frac{N}{L}[/tex]
so P is a distributed force (Newton/m), much like a beam problem.
Now, since this is an elastic phenomenon, I used Hooke's Law, saying that:
[tex]εE=\frac{PR}{t}=\frac{NR}{Lt} => N=\frac{εELt}{R}[/tex]
Let traction be fmax:
[tex]fmax=μN[/tex]
By combining the last two equations:
[tex]fmax=\frac{μεELt}{R}[/tex]
I would have been perfectly fine with this result, but for strains above ε=10^-6, this formula yields outlandishly high values of friction. For instance, for ε=0.7, I would get something like 0.4 GigaNewtons. I probably went wrong somewhere, but I really can't locate the mistake! I would be grateful for any advice you can give me!
P.S. All calculations were done in SI, so this is after the units check :P
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