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 h0:
p1=ρgh+ρgh0.
When the tube is placed horizontally, the trapped air only withstands the atmospheric pressure, temperature does not change, so
p1V1=p2V2,p2=p0,V2=V1p2p1.
Since the tube is of uniform cross-sectional area, we can replace volumes with heights because
V1,V2,...Vn↔Ah1,Ah2,...,Ahn.
Therefore:
h2=h1ρgh0ρgh+ρgh0= =h1h0h+h0=307616+76=36 cm. 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:
p1h1=p3h3,h3=h1p3p1,p3=p0−pm=ρgh−ρghm,h3=h1h0−hh+h0=3076−1616+76=46 cm.
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