Answer with Explanation:
The capillary rise in 2 parallel plates immersed in a liquid is given by the formula
[tex]h=\frac{2\sigma cos(\alpha )}{\rho gd}[/tex]
where
[tex]\sigma [/tex] is the surface tension of the liquid
[tex]\alpha [/tex] is the contact angle of the liquid
[tex]\rho [/tex] is density of liquid
'g' is acceleratioj due to gravity
'd' is seperation between thje plates
Part a) When the liquid is water:
For water and glass we have
[tex]\sigma =7.28\times 10^{-2}N/m[/tex]
[tex]\alpha =0 [/tex]
[tex]\rho _{w}=1000kg/m^3 [/tex]
Applying the values we get
[tex]h=\frac{2\times 7.28\times 10^{-2}cos(0)}{1000\times 9.81\times 2\times 10^{-3}}=7.39mm[/tex]
Part b) When the liquid is mercury:
For mercury and glass we have
[tex]\sigma =485.5\times 10^{-3}N/m[/tex]
[tex]\alpha =138^o [/tex]
[tex]\rho _{w}=13.6\times 10^{3}kg/m^3 [/tex]
Applying the values we get
[tex]h=\frac{2\times 485.5\times 10^{-3}cos(138)}{13.6\times 1000\times 9.81\times 2\times 10^{-3}}=-2.704mm[/tex]
The negative sign indicates that there is depression in mercury in the tube.