The problem I was trying to solve was this one.
Using the conservation of energy, I obtained that the velocity $v$ equals $$\sqrt{\frac{(2lx-x^2)g}{l-x}}$$
In the left segment, the momentum doesn't change, so the net force is zero. The reaction force on hinge A can be equated to the combined effect of the gravitational force and the thrust force(force due to changing mass) on the left segment of the chain . The thrust force is given by $$ \textbf{v}\frac{dm}{dt}$$
Here, the thrust force equals $k\frac{v^2}{2}$, where $k$ is the linear mass density. The $2$ in the denominator is because $$\frac{dm}{dt} = k\frac{d(x/2)}{dt}=k\frac{v}{2}$$
However, when we solve the problem this way, we arrive at a different answer than we would if approached using energy conservation. (Using energy conservation and $F=\frac{dp}{dt}$ for the system, we would get $R(x)=\frac{kg(2l^2+2lx-3x^2)}{4(l-x)}$)
In many such chain problems, using thrust force and energy conservation gives two different answers. Here's an example of another one.
A chain of length $L$ and mass per unit length $\rho$ is pulled on a horizontal surface. One end of the chain is lifted vertically with constant velocity $v$ by a force $P$. Find $P$ as a function of height $x$, and the work done by the force
My general doubt is: Why is there a discrepancy in answers? Which answer is more correct?