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Rolling cone motion is the rolling motion generated by a cone rolling over another cone. In rolling cone motion, at least one of the cones is convex , while the other cone may be either convex, or concave, or a flat surface (a flat surface can be regarded as a special case of a cone whose apex angle equals π {\displaystyle \pi } ).
In geometry, a polycon is a kind of a developable roller.It is made of identical pieces of a cone whose apex angle equals the angle of an even sided regular polygon. [1] [2] In principle, there are infinitely many polycons, as many as there are even sided regular polygons. [3]
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The larger the half angles of these cones the larger the axial force that the bearing can sustain. Tapered roller bearings are separable into a cone assembly and a cup. The non-separable cone assembly consists of the inner ring, the rollers, and a cage that retains and evenly spaces the rollers. The cup is simply the outer ring.
Rolling contact between a cylinder and a plane. Particles moving through the contact area from right to left, being strained more and more until local sliding sets in. Rolling contact problems are dynamic problems in which the contacting bodies are continuously moving with respect to each other.
When the cone angle is very small, the flow is nearly parallel everywhere in which case, an exact solution can be found, as shown by Theodore von Kármán and Norton B. Moore in 1932. [2] The solution is more apparent in the cylindrical coordinates ( ρ , ϖ , z ) {\displaystyle (\rho ,\varpi ,z)} (the ρ {\displaystyle \rho } here is the ...
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Conical spiral with an archimedean spiral as floor projection Floor projection: Fermat's spiral Floor projection: logarithmic spiral Floor projection: hyperbolic spiral. In mathematics, a conical spiral, also known as a conical helix, [1] is a space curve on a right circular cone, whose floor projection is a plane spiral.