The value of contact angle for kerosene with a solid surface.

(1) 0°

(2) 90°

(3) 45°

(4) 33° 

Nature of meniscus for liquid of $0^0$ angle of contact

(1) Plane

(2) Parabolic

(3) Semi-spherical

(4) Cylindrical

A liquid wets a solid completely. The meniscus of the liquid in a sufficiently long tube is 

(1) Flat

(2) Concave

(3) Convex

(4) Cylindrical

For which of the two pairs, the angle of contact is same

(1) Water and glass; glass and mercury

(2) Pure water and glass; glass and alcohol

(3) Silver and water; mercury and glass

(4) Silver and chromium; water and chromium

If the surface of a liquid is plane, then the angle of contact of the liquid with the walls of the container is -

(1) Acute angle

(2) Obtuse angle

(3) 90°

(4) 0°

If two soap bubbles of different radii are in communication with each other

(1) Air flows from larger bubble into the smaller one

(2) The size of the bubbles remains the same

(3) Air flows from the smaller bubble into the large one and the larger bubble grows at the expense of the smaller one

(4) The air flows from the larger

The surface tension of the soap solution is $25\times {10}^{-3} {\mathrm{Nm}}^{-1}$ . The excess pressure inside a soap bubble of diameter 1 cm is 

(1) 10 Pa

(2) 20 Pa

(3) 5 Pa

(4) None of the above

When two soap bubbles of radius ${\mathrm{r}}_1$ and ${\mathrm{r}}_2$ (${\mathrm{r}}_2$>${\mathrm{r}}_1$) coalesce, the radius of curvature of the common surface is

(1) ${\mathrm{r}}_2-{\mathrm{r}}_1$

(2)  $\frac{{\mathrm{r}}_2-{\mathrm{r}}_1}{{\mathrm{r}}_2{\mathrm{r}}_1}$

(3) $\frac{{\mathrm{r}}_2{\mathrm{r}}_1}{{\mathrm{r}}_2-{\mathrm{r}}_1}$

(4) ${\mathrm{r}}_2+{\mathrm{r}}_1$

A long cylindrical glass vessel has a small hole of radius 'r' at its bottom. The depth to which the vessel can be lowered vertically in the deep water bath (surface tension T) without any water entering inside is

(1) $4\mathrm{T}/\mathrm{r\rho g}$

(2) $3\mathrm{T}/\mathrm{r\rho g}$

(3) $2\mathrm{T}/\mathrm{r\rho g}$

(4) $\mathrm{T}/\mathrm{r\rho g}$

The excess of pressure inside a soap bubble than that of the outer pressure is

(1) $\frac{2\mathrm{T}}{\mathrm{r}}$

(2) $\frac{4\mathrm{T}}{\mathrm{r}}$

(3) $\frac{\mathrm{T}}{2\mathrm{r}}$

(4) $\frac{\mathrm{T}}{\mathrm{r}}$