When the tube is placed vertically with closed end down, the pressure of the trapped air withstands the pressure of the mercury "h" and of the air above mercury "h_0":
When the tube is placed horizontally, the trapped air only withstands the atmospheric pressure, temperature does not change, so
Since the tube is of uniform cross-sectional area, we can replace volumes with heights because
Therefore:
When we flip the tube and the closed end looks up, the trapped air pressure withstands 16 cm of mercury "pulling" down minus the atmospheric pressure "pushing" the mercury upward:
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