
To determine the density of the oil, we can utilize the fact that both arms of the U-tube are open to the atmosphere, leading to an equilibrium condition of pressures at the same horizontal level across both sides of the tube.
Consider the following points in the U-tube:
Since points B and C are at the same horizontal level, their pressures are equal. Therefore, the pressure exerted by the oil column must balance out the pressure exerted by the additional water column on the right side.
The pressure due to the oil column is:
P_{\text{oil}} = \rho_{\text{oil}} \cdot g \cdot h_{\text{oil}}
The pressure due to the extra water column is:
P_{\text{water}} = \rho_{\text{water}} \cdot g \cdot h_{\text{water}}
Where:
Equating the pressures from oil and water gives:
\rho_{\text{oil}} \cdot g \cdot 0.075 = 1000 \cdot g \cdot 0.065
Canceling out g and solving for \rho_{\text{oil}}:
\rho_{\text{oil}} = \dfrac{1000 \times 0.065}{0.075} = \dfrac{650}{0.75} = 866.67 \, \text{kg/m}^3
It seems there was a calculation error in the initial reasoning. This corrected calculation actually needs to be reevaluated considering the contribution of the oil's movement in the U-tube:
Re-examining the effective pressure equilibria we must ensure balancing including:
\rho_{\text{oil}} \cdot g \cdot 0.075 + \rho_{\text{water}} \cdot g \cdot 0.075 = 1000 \cdot g \cdot 0.065
Thus, check and resolve correctly might resolve around value approximations leading to answer below:
Given Statement: Choice aligns best with: