A thin tube of uniform cross section is sealed at both the ends. It lies horizontally, the middle 5 cm containing mercury and the parts on its two sides containing air at the same pressure P. When the tube is held at an angle of 60∘ with the vertical, the length of the air column above and below the mercury pellet are 46 cm and 44.5 cm respectively. Calculate the pressure P, if the temperature of the system is kept at 30∘C.
When the tube is kept inclined to the vertical, the length of the upper part is l1=46 cm, and that of the lower part is l2=44.5 cm. When the tube lies horizontally, the length on each side is -
l0=[l1+l22]=[46 +44.5 2]=45.25 cm.
Let P1 and P2 be the pressures in the upper and the lower parts when the tube is kept inclined. As the temperature is constant throughout, we can apply Boyle's law.
For the upper part,
P1l1A=Pl0A
⇒P1=(Pl0l1)....(i).
Similarly, for the lower part,
P2=(Pl0l2)....(ii).
Thus,
P2=P1+mgAcos 60∘.
Putting from (i) and (ii),
(Pl0l2)=(Pl0l1)+(mg2A)
⇒Pl0(1l2−1l1)=mg2A
⇒P=⎡⎢
⎢
⎢
⎢⎣mg2Al0(1l2−1l1)⎤⎥
⎥
⎥
⎥⎦.
If the pressure P is equal to a height h of mercury,
P=ρgh.
Also mas of the mercury pellet is m=(5 cm)Aρ
⇒ρgh=⎡⎢
⎢
⎢
⎢⎣(5 cm)Aρg2Al0(1l2−1l1)⎤⎥
⎥
⎥
⎥⎦
⇒h=⎡⎢
⎢
⎢
⎢⎣(5)2×(45.25)×(144.5−146)⎤⎥
⎥
⎥
⎥⎦=75.4 cm.
The pressure P is equal to 75.4 cm of Hg.