Gh778
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Gh778 said:How can I do ?
Like the drawing ? maybe sin(a)+cos(a) ?
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it's an internet drawing ;)By the way, your software is great and of course you are so good in using it.
Gh778 said:I confused, I don't understand your last message, what's dv, du ?
If you divided by 2 proof, you divided by 4 the torque because surface is half and pressure is half. With square thread, not exactly divided by 4 because the thread is square (depend of the start and end).I think if we make uLimit half, the torque becomes half too.
The upper surface is for example d=0 rd and the lower surface is with d=-0.5 rd. This is what I said there is a torque (I take upper torque less lower torque).How about the lower surface.
For you the result in my program is not fine ? You suppress sin and cos ?First, In you code, in general, a=atan(1/v) . But for 2pi span, the result is fine. The equation for local torque is then simplified to Torque=(uLimit-u)/10*pas*pas.
For me the force on the gasket can be near zero. Except the problem of capillary action we can take the film very low as possible. And the square thread fixed the gasket on it so the deformation can be limited. It's only a technical problem.Also remember that the gasket is elastic. If the torque or force from one side causes deformation it, it applies a force on the surface.
But there is a vertical force if we put only water at up surface. Vertical force is cancel with up and down surface only. The study is with up and down surfaces with water. The vertical force don't care about radius. If up and down surface have water, the up/down forces on gasket is 0.Just imagine that there is no water in the lower gap but the gasket is there. The upper force or torque deform the gasket till the thread comes to equilibrium. The force of the gasket would be as large as the hydraulic force
Not at all, the upper force is give with square thread when d = 0 rd. The lower force is give with square thread when d=-0.5 rd (it's an example).You just calculated a net force due to the upper water.