Let
A be the area of the cross section of the tube and
l be the length of the tube. Then initial volume of air inside tube is
V1=Al and initial pressure is
Po (atmospheric pressure).
When the tube is immersed in liquid to a distance
x, then level of liquid inside and outside are same as shown in figure. Now volume of air inside the tube is
V2=A(l−x) and pressure inside the tube is
P2=Po+2Tr According to Boyle's law, we have
PoAl=(Po+2Tr)A(l−x)⇒x=l(1+rPo2T)
on substituting the values, we have
x=0.11(1+10−5×1.012×1052×5.06×10−2)=0.01m=1cm
When the seal is broken, pressure inside the tube is equal to atmospheric and rise of liquid through h in the tube is given by, hρg=2Tr
⇒h=2Trρg, on substituting the values, we have
⇒h=2×5.06×10−210−5×1000×9.8=1.03m
but length of the tube outside liquid is (l−x)=(0.11−0.01)m=0.1m, so the tube will be of insufficient length. So the liquid will rise to the top.