Initially,
Length of the narrow bore, L=1 m=100 cm
Length of the mercury thread, l=76 cm
Length of the air column trapped between mercury and the closed end, x=15 cm
Air column at the top =100−(76+15)=9 cm
Initial pressure of air trapped, P1=Pa=76 cm of mercury
Taking cross section of the bore to be 𝐴,
Initial volume of air,
V1=A×x=15 A cm3
Now, the bore is held vertically in air with the open end at the bottom, the mercury length that occupies the air space is:
100–(76+15)=9 cm
Hence, the total length of the air column =15+9=24 cm.
Let h cm of mercury flow out as a result of atmospheric pressure.
Length of the air column in the bore, y=(24+h) cm
And, length of the mercury column remaining =(76−h) cm
Final pressure, P2=Pa−(76−h)=76−(76−h)=h cm of mercury
Final volume of air,
V2=A×y=(24+h)A cm3
Temperature remains constant throughout the process.
Therefore, applying Boyle’s law,
P1V1=P2V2
⇒76×15A=h(24+h)A
⇒h2+24h−1140=0
Using quadratic formula,
h=−24±√242+4×1×11402
=23.8 cm or −47.8 cm
Height cannot be negative.
Hence, 23.8 cm of mercury will flow out from the bore.
Remaining column of mercury =76−23.8=52.2 cm.
The length of the air column will be 24+23.8=47.8 cm.