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A body P floats in water with half its v...

A body P floats in water with half its volume immersed. Another body Q floats in a liquid of density `(3)/(4)`th of the density of water with two - third of the volume immersed. The ratio of density of P to that of Q is

A

`1:2`

B

`1:1`

C

`2:3`

D

`3:4`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we will use Archimedes' principle, which states that the buoyant force acting on a body immersed in a fluid is equal to the weight of the fluid displaced by the body. ### Step-by-Step Solution: 1. **Identify the given information:** - Body P floats in water with half its volume immersed. - Body Q floats in a liquid with density \( \frac{3}{4} \) of the density of water, with two-thirds of its volume immersed. 2. **Define the variables:** - Let the volume of body P be \( V_P \). - Let the density of body P be \( \rho_P \). - Let the density of water be \( \rho_W \). - Let the volume of body Q be \( V_Q \). - Let the density of body Q be \( \rho_Q \). 3. **Apply Archimedes' principle for body P:** - The weight of body P is equal to the buoyant force acting on it. - The volume of body P that is immersed is \( \frac{V_P}{2} \). - The buoyant force is given by: \[ \text{Buoyant Force} = \text{Weight of liquid displaced} = \left(\frac{V_P}{2}\right) \rho_W g \] - The weight of body P is: \[ \text{Weight of P} = V_P \rho_P g \] - Setting these equal gives: \[ V_P \rho_P g = \left(\frac{V_P}{2}\right) \rho_W g \] - Canceling \( V_P g \) from both sides (assuming \( V_P \neq 0 \) and \( g \neq 0 \)): \[ \rho_P = \frac{\rho_W}{2} \] 4. **Apply Archimedes' principle for body Q:** - The volume of body Q that is immersed is \( \frac{2V_Q}{3} \). - The buoyant force is given by: \[ \text{Buoyant Force} = \text{Weight of liquid displaced} = \left(\frac{2V_Q}{3}\right) \left(\frac{3}{4} \rho_W\right) g \] - The weight of body Q is: \[ \text{Weight of Q} = V_Q \rho_Q g \] - Setting these equal gives: \[ V_Q \rho_Q g = \left(\frac{2V_Q}{3}\right) \left(\frac{3}{4} \rho_W\right) g \] - Canceling \( V_Q g \) from both sides (assuming \( V_Q \neq 0 \) and \( g \neq 0 \)): \[ \rho_Q = \frac{2}{3} \cdot \frac{3}{4} \rho_W = \frac{1}{2} \rho_W \] 5. **Find the ratio of densities \( \rho_P \) and \( \rho_Q \):** - From the previous steps, we have: \[ \rho_P = \frac{\rho_W}{2} \] \[ \rho_Q = \frac{\rho_W}{2} \] - Therefore, the ratio of the densities is: \[ \frac{\rho_P}{\rho_Q} = \frac{\frac{\rho_W}{2}}{\frac{\rho_W}{2}} = 1 \] 6. **Conclusion:** - The ratio of the density of body P to the density of body Q is \( 1:1 \).
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