Hello, I need help with this problem of applied dynamics $2)$ A shipping container is suspended from a crane by an inextensible cable. The crane rotates in the vertical plane at the constant angular speed $\backslash (\backslash$Omega $\backslash ).$ It may be assumed that the cable remsins taut, $50$ its orientation is describable in terms of the angle $\backslash (\backslash$theta $\backslash )$ locating the vertical plane in which it is situated relative to the plane of the crane and the angle of elevation $\backslash (\backslash$phi $\backslash )$ from a vertical line. Based on a model of the container as a small particle, and having $\backslash (\backslash$theta $\backslash )$ and $\backslash (\backslash$phi $\backslash )$ as the only unknowis, derive:

a$)$ the acceleration of the coutainer

b$)$ the differential equations of motion $($apply Newton's $2$nd law to the coutainer$)2)$ A shipping container is suspended from a crane by an inextensible cable. The crane rotates in the vertical plane at the constant angular speed $\backslash (\backslash$Omega $\backslash ).$ It may be assumed that the cable remsins taut, $50$ its orientation is describable in terms of the angle $\backslash (\backslash$theta $\backslash )$ locating the vertical plane in which it is situated relative to the plane of the crane and the angle of elevation $\backslash (\backslash$phi $\backslash )$ from a vertical line. Based on a model of the container as a small particle, and having $\backslash (\backslash$theta $\backslash )$ and $\backslash (\backslash$phi $\backslash )$ as the only unknowis, derive:

a$)$ the acceleration of the coutainer

b$)$ the differential equations of motion $($apply Newton's $2$nd law to the coutainer$)$