To determine the density of the liquid in which the block of wood just floats, we use the principle of flotation. According to this principle, the weight of the fluid displaced by the submerged part of the block is equal to the weight of the block.
Given that the block floats in water with $\frac{4}{5}$ of its volume submerged, the density of water is $\rho_w = 1000 \, \text{kg/m}^3$, and the following relationship holds:
$\rho_{block} \cdot V_{block} = \rho_{water} \cdot V_{submerged}$
where
Thus, the weight balance in water is:
$\rho_{block} = \frac{\rho_{water} \cdot \frac{4}{5} V_{block}}{V_{block}} = \frac{4}{5} \cdot \rho_w$
In this case,
$\rho_{block} = \frac{4}{5} \cdot 1000 = 800 \, \text{kg/m}^3$
Now, when the block floats in a different liquid, such that it just floats, the density of the liquid ($\rho_{liquid}$) equals the density of the block, which is:
$\rho_{liquid} = \rho_{block} = 800 \, \text{kg/m}^3$
Thus, the density of the liquid is 800 kg/m3.
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: