Step 1: State the law of floatation.
A floating body displaces fluid equal to its own weight. When a body floats: \[ \text{Weight of body} = \text{Weight of fluid displaced} = \rho_{\text{fluid}} \times V_{\text{submerged}} \times g \] This is Archimedes principle applied to floating objects.
Step 2: Apply the floating condition in water to find the density of wood.
Let $\rho_w$ be the density of wood and $V$ be its total volume. Half the volume is submerged in water ($\rho_{\text{water}} = 1000 \, \text{kg m}^{-3}$): \[ \rho_w \cdot V \cdot g = \rho_{\text{water}} \cdot \frac{V}{2} \cdot g \] Cancelling $Vg$ from both sides: \[ \rho_w = \frac{\rho_{\text{water}}}{2} = \frac{1000}{2} = 500 \, \text{kg m}^{-3} \]
Step 3: Understand why only half is submerged.
The fraction submerged equals the ratio of the body's density to the fluid's density: \[ \text{fraction submerged} = \frac{\rho_{\text{body}}}{\rho_{\text{fluid}}} = \frac{500}{1000} = \frac{1}{2} \] A body with half the fluid's density floats with exactly half its volume submerged. This is a general and very useful rule.
Step 4: Apply the floating condition in oil.
In oil, $0.8V$ of the wood's volume is submerged. Let $\rho_o$ be the density of the oil: \[ \rho_w \cdot V \cdot g = \rho_o \cdot 0.8V \cdot g \] Cancelling $Vg$: \[ \rho_w = 0.8 \rho_o \]
Step 5: Solve for the density of oil.
\[ 500 = 0.8 \rho_o \] \[ \rho_o = \frac{500}{0.8} = 625 \, \text{kg m}^{-3} \]
Step 6: Verify using the fraction-submerged rule.
Fraction submerged in oil $= \rho_w / \rho_o = 500/625 = 0.8$, which matches the given condition that $0.8V$ is submerged. The oil is less dense than water (625 vs 1000), so a greater fraction of the wood must submerge in oil to displace enough weight, which is physically consistent. \[ \boxed{\rho_{\text{oil}} = 625 \, \text{kg m}^{-3}} \]