Step 1: Trace the fluid path between the two points.
P sits at the top of the water column and Q is the open end above the mercury leg. Between them the tube carries a water column of height \(h_1\), then an oil-filled loop with a net rise of \(h_2\), then a mercury column of height \(h_3\) up to Q.
Step 2: Write the pressure balance starting from the open end.
At Q the gauge pressure is zero. Moving down through mercury by \(h_3\) adds pressure, then moving back up through oil by \(h_2\) and through water by \(h_1\) removes pressure on the way to P. So \(P_P = \rho_{Hg} g h_3 - \rho_{oil} g h_2 - \rho_{w} g h_1\).
Step 3: Substitute the numbers.
With \(\rho_{Hg} = 13600\) kg/m\(^3\), \(\rho_{oil} = 900\) kg/m\(^3\), \(\rho_w = 1000\) kg/m\(^3\) and \(g = 10\) m/s\(^2\): \(\rho_{Hg} g h_3 = 13600 \times 10 \times 0.8 = 108800\) Pa, \(\rho_{oil} g h_2 = 900 \times 10 \times 0.7 = 6300\) Pa, \(\rho_w g h_1 = 1000 \times 10 \times 0.5 = 5000\) Pa.
Final Answer:
\(P_P = 108800 - 6300 - 5000 = 97500\) Pa, so the gauge pressure at P is 97.5 kPa, which sits inside the official 95 to 98 kPa band.
\[ \boxed{P_P = 97.5 \text{ kPa}} \]