Original Post
How do I break down a force applied at a specific point on a two-dimensional rigid body into its resultant linear and angular products with relation to said body? It makes sense to me that if the force pierces the center of mass of the body, no torque is induced. Likewise for forces that act on the body as a whole, like gravity or buoyancy. Am I right in these assertions? The direction I've gone is something like this: Given a body with a center of mass c, a force f at point p- I find a line segment s perpindicular to f that connects c to a point on the body's edge. The bisection of s represents the partitioning of the force. If f pierces the center of mass 100% linear acceleration is the result. If instead f pierces the point on the body's edge, 100% angular acceleration is induced. If the segment is cut in half, 50% linear and 50% angular and so on... Am I laughably off track? It seems like an awfully rudimentary axiom- but then all of physics is (beatifully) absurd abstractions, no? I'm relatively new to physics and get most frustrated with the symbology/language; never the concept itself... so hand-holding is appreciated! Thanks