Surface Tension
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361229 A glass tube of uniform internal radius (\(r\)) has a valve separating the two identical ends. Initially, the valve is in a tightly closed position. End 1 has a hemispherical soap bubble of radius \(r\). End 2 has sub-hemispherical soap bubble of radius \(r\) as shown in figure. Just after opening the valve.
supporting img

1 Air from end 1 flows towards end 2. No change in the volume of the soap bubbles
2 Air from end 1 flows towards end 2. Volume of the soap bubble at end 1 decreases
3 No change occurs
4 Air from end 2 flows towards end 1. Volume of the soap bubble at end 1 increases.
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361230 The excess pressure inside a spherical drop of water is four times that of another drop. Then their respective mass ratio is

1 \(1: 16\)
2 \(8: 1\)
3 \(1: 4\)
4 \(1: 64\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361231 Two soap bubbles of radii \(r_{1}\) and \(r_{2}\) equal to \(4\;cm\) and \(5\;cm\) are touching each other over a common surface \({S_1}\;{S_2}\) (shown in figure ). Its radius will be
supporting img

1 \(4\;cm\)
2 \(20\;cm\)
3 \(5\;cm\)
4 \(4.5\;cm\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361232 Two soap bubbles coalesce. It is noticed that, whilst Joined together, the radii of the two bubbles are \(a\) and \(b\) where \(a>b\). Then, the radius of curvature of interface between the two bubbles will be

1 \(a-b\)
2 \(a+b\)
3 \(\dfrac{a b}{(a-b)}\)
4 \(\dfrac{a b}{(a+b)}\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361229 A glass tube of uniform internal radius (\(r\)) has a valve separating the two identical ends. Initially, the valve is in a tightly closed position. End 1 has a hemispherical soap bubble of radius \(r\). End 2 has sub-hemispherical soap bubble of radius \(r\) as shown in figure. Just after opening the valve.
supporting img

1 Air from end 1 flows towards end 2. No change in the volume of the soap bubbles
2 Air from end 1 flows towards end 2. Volume of the soap bubble at end 1 decreases
3 No change occurs
4 Air from end 2 flows towards end 1. Volume of the soap bubble at end 1 increases.
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361230 The excess pressure inside a spherical drop of water is four times that of another drop. Then their respective mass ratio is

1 \(1: 16\)
2 \(8: 1\)
3 \(1: 4\)
4 \(1: 64\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361231 Two soap bubbles of radii \(r_{1}\) and \(r_{2}\) equal to \(4\;cm\) and \(5\;cm\) are touching each other over a common surface \({S_1}\;{S_2}\) (shown in figure ). Its radius will be
supporting img

1 \(4\;cm\)
2 \(20\;cm\)
3 \(5\;cm\)
4 \(4.5\;cm\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361232 Two soap bubbles coalesce. It is noticed that, whilst Joined together, the radii of the two bubbles are \(a\) and \(b\) where \(a>b\). Then, the radius of curvature of interface between the two bubbles will be

1 \(a-b\)
2 \(a+b\)
3 \(\dfrac{a b}{(a-b)}\)
4 \(\dfrac{a b}{(a+b)}\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361229 A glass tube of uniform internal radius (\(r\)) has a valve separating the two identical ends. Initially, the valve is in a tightly closed position. End 1 has a hemispherical soap bubble of radius \(r\). End 2 has sub-hemispherical soap bubble of radius \(r\) as shown in figure. Just after opening the valve.
supporting img

1 Air from end 1 flows towards end 2. No change in the volume of the soap bubbles
2 Air from end 1 flows towards end 2. Volume of the soap bubble at end 1 decreases
3 No change occurs
4 Air from end 2 flows towards end 1. Volume of the soap bubble at end 1 increases.
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361230 The excess pressure inside a spherical drop of water is four times that of another drop. Then their respective mass ratio is

1 \(1: 16\)
2 \(8: 1\)
3 \(1: 4\)
4 \(1: 64\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361231 Two soap bubbles of radii \(r_{1}\) and \(r_{2}\) equal to \(4\;cm\) and \(5\;cm\) are touching each other over a common surface \({S_1}\;{S_2}\) (shown in figure ). Its radius will be
supporting img

1 \(4\;cm\)
2 \(20\;cm\)
3 \(5\;cm\)
4 \(4.5\;cm\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361232 Two soap bubbles coalesce. It is noticed that, whilst Joined together, the radii of the two bubbles are \(a\) and \(b\) where \(a>b\). Then, the radius of curvature of interface between the two bubbles will be

1 \(a-b\)
2 \(a+b\)
3 \(\dfrac{a b}{(a-b)}\)
4 \(\dfrac{a b}{(a+b)}\)
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361229 A glass tube of uniform internal radius (\(r\)) has a valve separating the two identical ends. Initially, the valve is in a tightly closed position. End 1 has a hemispherical soap bubble of radius \(r\). End 2 has sub-hemispherical soap bubble of radius \(r\) as shown in figure. Just after opening the valve.
supporting img

1 Air from end 1 flows towards end 2. No change in the volume of the soap bubbles
2 Air from end 1 flows towards end 2. Volume of the soap bubble at end 1 decreases
3 No change occurs
4 Air from end 2 flows towards end 1. Volume of the soap bubble at end 1 increases.
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361230 The excess pressure inside a spherical drop of water is four times that of another drop. Then their respective mass ratio is

1 \(1: 16\)
2 \(8: 1\)
3 \(1: 4\)
4 \(1: 64\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361231 Two soap bubbles of radii \(r_{1}\) and \(r_{2}\) equal to \(4\;cm\) and \(5\;cm\) are touching each other over a common surface \({S_1}\;{S_2}\) (shown in figure ). Its radius will be
supporting img

1 \(4\;cm\)
2 \(20\;cm\)
3 \(5\;cm\)
4 \(4.5\;cm\)
PHXI10:MECHANICAL PROPERTIES OF FLUIDS

361232 Two soap bubbles coalesce. It is noticed that, whilst Joined together, the radii of the two bubbles are \(a\) and \(b\) where \(a>b\). Then, the radius of curvature of interface between the two bubbles will be

1 \(a-b\)
2 \(a+b\)
3 \(\dfrac{a b}{(a-b)}\)
4 \(\dfrac{a b}{(a+b)}\)