Explanations & Calculations
- As stated in the question all the contacts are smooth, thus friction neither supports nor restrict the motion of the two-mass system.
- Understand the situation that if the masses are left at rest, "\\small 2m" will drag the thread downwards & the thread will drag "\\small m" downwards through the hole. If there was some friction, it would have opposed this motion & kept them in rest.
- Since it is not, the mass "\\small m" needs to move in a circle on the table which can support & keep "\\small 2m" in place without falling down.
- Keeping a sufficient uniform speed, keeps "\\small 2m" stable whereas too low speeds cause "\\small 2m" go down & too much speed causes "\\small 2m" goes up & eventually breaking the stability.
- Centripetal force & the fictitious centrifugal force on m support this behavior.
- During this motion, mass "\\small 2m" is in vertical equilibrium, which leads to the possibility of writing, "\\small \\uparrow T= \\downarrow2mg\\cdots(1)"
- Since mass "\\small m" is in circular motion, Newton's second law can be applied on "\\small m" towards the center of the 1m circle.
"\\qquad\\qquad\n\\begin{aligned}\n\\small F&= \\small ma\\implies T=m\\frac{v^2}{r}=m\\frac{v^2}{1}=mv^2\\cdots (2)\\\\\n\\small \n\\end{aligned}"
"\\qquad\\qquad\n\\begin{aligned}\n\\small 2mg&= mv^2\\\\\n\\small v^2 &= \\small 2g\\cdots(\\because\\cancel{m})\\\\\n\\small\\bold{v}&= \\small \\bold{\\sqrt{2g}}\n\\end{aligned}"
- This is the sufficient magnitude of the speed.
Comments
Leave a comment