Two blocks of equal mass m are connected by a flexible inelastic cord of mass M. One block is placed on a smooth horizontal table, the other block hangs over the edge. The total potential energy of the entire cord is given by (−Mg, where x is the distance of the hanging block from the edge of the table, l is the length of the cord, and g is the gravitational acceleration. Then
Part BCSIR NET December 2024the-whole-system-shares-the-acceleration
The whole system shares the acceleration
Related counterexample: The generalised momentum ∂L/∂q̇ always equals mass × velocity
- Part B questionDecember 2023
- x is cyclic so its equation is a conservation lawDecember 2024
- the radial inertia term vanishes with r dotDecember 2024
- the cross term changes the effective inertiaDecember 2024
- parallel axis shift forgottenJune 2024
- the jacobian adds a power of rJune 2024
The chapter behind this: Lagrangian mechanics — free to read
From Classical Mechanics › Lagrangian formalism and generalised coordinates