I am having trouble understanding how radial force works. I am working in a dynamics course so there's always centripetal acceleration.
My difficulty comes from two cases.
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Analyzing a car traveling over a hill, it crosses the peak at maximum possible speed (Normal force is 0 N). Here my professors vector diagram had only weight downwards and no radial force.
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A helical slide, having a person traveling down. Here I was asked to work out a radial force which is equal to $mv^2/R$.
My question is why was there no radial force included when the car traveled over the top of the hill, why there is a radial force in case 2 and most importantly, when will there be a radial force?
Best Answer
I consider it helpful to include the phrase "... acts as central force" when talking/thinking about such problems.
There are many forces (gravity, tension in a string, ...) that may or may not act as a central force.
Considering your examples: