$A$ vertical glass capillary tube of radius $r$ open at both ends contains some water (surface tension $T$ and density $\rho$). If $L$ be the length of the water column,then:

  • A
    $L=\frac{4 T}{r \rho g}$
  • B
    $L=\frac{2 T}{r \rho g}$
  • C
    $L=\frac{T}{4 r \rho g}$
  • D
    $L=\frac{T}{2 r \rho g}$

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$A$ capillary tube of radius '$r$' is immersed in water and water rises to a height of '$h$'. The mass of water in the capillary tube is $5 \times 10^{-3} \ kg$. The same capillary tube is now immersed in a liquid whose surface tension is $\sqrt{2}$ times the surface tension of water. The angle of contact between the capillary tube and this liquid is $45^{\circ}$. The mass of liquid which rises into the capillary tube now is (in $kg$):

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