Problem Explanation:
The problem involves two liquids with different densities (ρ1\rho_1ρ1 and ρ2\rho_2ρ2) and requires determining the depth from the free surface where the pressure remains the same (PPP) after replacing the liquid.
Key Concepts:
Hydrostatic Pressure Formula:
P=Patm+ρghP = P_{\text{atm}} + \rho g hP=Patm+ρghwhere:
- PPP: Pressure at a depth hhh.
- PatmP_{\text{atm}}Patm: Atmospheric pressure acting on the free surface.
- ρ\rhoρ: Density of the liquid.
- ggg: Acceleration due to gravity.
- hhh: Depth from the free surface.
In both cases, PPP remains the same, and PatmP_{\text{atm}}Patm is constant.
Given:
In the first liquid (ρ1\rho_1ρ1):
P=Patm+ρ1gh1P = P_{\text{atm}} + \rho_1 g h_1P=Patm+ρ1gh1where h1=hh_1 = hh1=h (depth of point AAA).
In the second liquid (ρ2\rho_2ρ2): Let the depth from the free surface at which the pressure is PPP be h2h_2h2. The pressure equation becomes:
P=Patm+ρ2gh2P = P_{\text{atm}} + \rho_2 g h_2P=Patm+ρ2gh2
Solution:
Since the pressure PPP and PatmP_{\text{atm}}Patm are the same in both cases:
ρ1gh1=ρ2gh2\rho_1 g h_1 = \rho_2 g h_2ρ1gh1=ρ2gh2
Canceling ggg (as gravity is constant) and substituting h1=hh_1 = hh1=h:
ρ1h=ρ2h2\rho_1 h = \rho_2 h_2ρ1h=ρ2h2
Solving for h2h_2h2:
h2=ρ1ρ2hh_2 = \frac{\rho_1}{\rho_2} hh2=ρ2ρ1h
Final Answer:
The depth from the free surface where the pressure is PPP after replacing the liquid is:
h2=ρ1ρ2hh_2 = \frac{\rho_1}{\rho_2} hh2=ρ2ρ1h
Notes:
- If ρ2>ρ1\rho_2 > \rho_1ρ2>ρ1, h2<hh_2 < hh2<h (the point moves closer to the surface).
- If ρ2<ρ1\rho_2 < \rho_1ρ2<ρ1, h2>hh_2 > hh2>h (the point moves deeper into the liquid).