Atmospheric pressure supports liquid column:
$$P_\text{atm} = \rho g h$$ $$h = \frac{P_\text{atm}}{\rho g}$$
\(h_\text{Hg} = 0.76\) m
Supports \(P_\text{atm}\)
\(h_\text{wine} = ?\)
Same \(P_\text{atm}\)
Method 1: Density ratio (simplest)
$$\frac{h_\text{wine}}{h_\text{Hg}} = \frac{\rho_\text{Hg}}{\rho_\text{wine}}$$ $$h_\text{wine} = 0.76 \times \frac{13{,}600}{984} = 0.76 \times 13.82 = 10.50 \, \text{m}$$
Method 2: Direct pressure
$$h_\text{wine} = \frac{1.013 \times 10^5}{984 \times 9.8} = \frac{1.013 \times 10^5}{9643} \approx 10.51 \, \text{m}$$
\(h = \textbf{10.5 m}\)
Pascal used red wine, observed ~10 m column, confirming Torricelli's vacuum above liquid.