Links to Questions
Thursday, June 14, 2012
Kerala Engineering Entrance 2012 (KEAM Engg. 2012) Questions on Surface Tension
Wednesday, July 14, 2010
EAMCET 2010 Questions (MCQ) on Surface Tension
Today we will discuss two questions on surface tension which appeared in EAMCET 2010 question papers.
The following multiple choice question appeared in EAMCET 2010 (Engineering) question paper:
The excess pressure inside a spherical soap bubble of radius 1 cm is balance by a column of oil (Sp. gravity 0.8) 2 mm high. The surface tension of oil is
(1) 3.92 N/m
(2) 0.0392 N/m
(3) 0. 392 N/m
(4) 0.00392 N/m
The excess pressure ∆P insie a spherical bubble of radius r is given by
∆P = 4 T/r where T is the surface tension.
The pressure p exerted by a liquid column of height h is given by
p = hρg where ρ is the density of the liquid.
Therefore we have
4 T/r = hρg from which T = rhρg/4
Substituting for known values, T = (1×10–2×2×10–3×0.8×103×10)/4 = 0.004 N/m [Option (4)].
[If you substitute g = 9.8 ms–2 instead of 10 ms–2 (as we did above for convenience), you will get the answer as 0.00392 N/m].
Here is the question which appeared in EAMCET 2010 (Agriculture and Medicine) question paper:
A spherical liquid drop of diameter D breaks up to n identical spherical drops. If the surface tension of the drop is ‘σ’, the change in energy in this process is
(1) πσD2(n1/3 – 1)
(2) πσD2(n2/3 – 1)
(3) πσD2(n – 1)
(4) πσD2(n4/3 – 1)
The surface energy (E1) of a drop of radius R is given by
E1 = 4πR2σ
Or E1 = πD2σ where D is the diameter of the drop.
When a drop of radius R breaks into n identical droplets, the radius r of each droplet is given by (on equating the volumes)
(4/3) πR3 = n×(4/3) πr3
Therefore, r = R/n1/3
The total surface energy (E2) of all the n droplets is given by
E2 = n×4πr2σ = n×4π (R/n1/3) 2σ = 4πR2σn1/3
Or, E2 = πD2σn1/3
The change in energy is E2 – E1 = πσD2(n1/3 – 1)
Wednesday, April 04, 2007
Surface Tension–Questions involving excess of pressure inside a bubble
Here is a question which is popular among question setters:
Two spherical soap bubbles of radii r1 and r2 in vacuum combine under isothermal conditions. The resulting bubble has a radius equal to
(a) (r1+r2)/2 (b) √(r1+r2) (c) r1r2/(r1+r2) (d) (r1+r2)/√2 (e) √(r12+r22)
As the temperature is constant, we have P1V1+ P2V2 =.PV where P1 and P2 are the pressures inside the separate bubbles, V1 and V2 are their volumes, P is the pressure inside the combined bubble and V is its volume.
Since the bubbles are located in vacuum, the pressure inside the bubble is equal to the excess of pressure 4T/r, where T is the surface tension and ‘r’ is the radius so that we have (4T/r1)×[(4/3)πr13]+ (4T/r2)×[(4/3)πr23] = (4T/R)×[(4/3)πR3] where R is the radius of the combined bubble.
This yields R = √(r12+r22).
[You can work out this problem by equating the surface energies: 4πr12T+4πr22T= 4πR2T, from which R = √(r12+r22)]
Now, consider the following MCQ:
Excess of pressure inside one soap bubble is four times that inside another. Then the ratio of the volume of the first bubble to that of the second is
(a) 1:16 (b) 1:32 (c) 1:64 (d) 1:2 (e) 1:4
If r1 and r2 are the radii of the bubbles and T is the surface tension of soap solution, we have (4T/r1)/(4T/r2) = 4.
Therefore, r1/r2 = ¼. Since the volume is directly proportional to the cube of the radius, the ratio of volumes V1/V2 = (r1/r2)3 = (¼)3 = 1/64 [Option (d)].
The following MCQ appeared in AIEEE 2004 question paper. This question is popular among question setters and has appeared in other entrance test papers as well:
If two soap bubbles of different radii are connected by a tube,
(a) air flows from the bigger bubble to the smaller bubble till the sizes become equal
(b) air flows from the bigger bubble to the smaller bubble till the sizes are interchanged
(c) air flows from the smaller bubble to the bigger
The excess of pressure inside the smaller bubble is greater than that inside the bigger bubble. (Remember, P = 4T/r and hence excess of pressure ‘P’ is inversely proportional to the radius ‘r’). Therefore, air will flow from the smaller bubble to the bigger bubble [Option (c)].
Tuesday, September 19, 2006
Properties of Fluids
Application of Bernoulli’s theorem can be seen in
(a) dynamic lift of aeroplane (b) hydraulic press (c) helicopter (d) none of these
The correct option is (a). The shape of the aeroplane wings is such that when it moves forward, the air molecules at the top of the wings have a greater velocity (relative to the wings) compared to the air molecules at the bottom. Therefore, in accordance with Bernoulli’s principle, the pressure at the top of the wings is less than that at the bottom. This results in a dynamic lift of the wings which balances the weight of the plane.
Let us now consider another question involving Bernoulli’s principle:
Water is flowing steadily through two horizontal pipes of radii 3cm and 6cm connected in series. The speed of water in the first pipe is 2m/s and the pressure of water in it is 2×104 pascal. The pressure of water in the second pipe will be nearly
(a) 2×104 pascal (b) 2.2×104 pascal (c) 2.4×104 pascal (d) 2.6×104 pascal (e) 3×104 pascal
The speed v2 of water in the second pipe is given (from the equation of continuity, a1v1 = a2v2 ) by v2 = 2×a1/a2 = 2×1/4 = 0.5 m/s. (The ratio of cross section areas is ¼ since the radius of the second pipe is twice that of the first).
As per Bernoulli’s principle, we have P1 + (ρv12 )/2 + ρgh = P2 + (ρv22)/2 + ρgh with usual notations. Therefore, P2 = P1 + ρ(v12- v22)/2 =2×104 + 1000(22 – 0.52)/2 = 2.1875×104 pascal. The correct option therefore is (b).
The following question involving surface tension may appear to be difficult for some of you. See how simple it is:
Two soap bubbles of radii ‘R’ and ‘r’ (R > r) are touching each other. The radius of curvature of the common surface at the region of contact is
(a) (R+r)/2 (b) R – r (c) (R – r)/2 (d) Rr/(R+r) (e) Rr/(R-r)
At the contact region, the radius of curvature (R') of the soap film is governed by the net excess of pressure 4T/r – 4T/R where T is the surface tension. Therefore, we have 4T/r – 4T/R = 4T/R' from which R' = Rr/R-r [option (e)].
Consider now the following M.C.Q.:
Two rain drops are falling through air with the same terminal velocity of 8cm/s. If they coalesce, the terminal velocity of the combined single drop will be (in cm/s)
(a) 8/√2 (b) 16 (c) 8×41/3 (d) 8×21/3 (e) 8√2
On equating the apparent weight of a rain drop to the viscous force (air resistance) opposing the downward motion of the drop, we have, 4/3πr3(ρ-σ)g = 6πrηv, with usual notations. Therefore, the velocity, v α r2…………(1)
Since the drops have the same terminal velocity, it follows that they have the same radius. The radius (r1 ) of the single large drop (when the two drops coalesce) is given by
2× 4/3πr3 = 4/3 πr13. Therefore, r1=21/3 r.
The velocity of the combined single drop, v1 α [21/3 r]2 -------------- (2)
Wednesday, August 09, 2006
Questions on Surface Tension
You might be remembering the expression for the excess of pressure ‘p’ inside a liquid drop: p = 2T/r where ‘T’ is the surface tension of the liquid and ‘r’ is the radius of the drop. The excess pressure is due to surface tension by which the free surface of a liquid behaves like a stretched membrane. The excess of pressure inside a bubble is 4T/r, which is twice that inside a drop because a bubble has two free surfaces (inner and outer).
Consider the following question which often finds a place in Medical and Engineering Entrance test papers:
Two soap bubbles A and B are obtained at the ends of a glass tube with a stop cock at its middle. The stop cock is closed initially and the bubble B is larger in size. If the stop cock is opened what happens to the bubbles?
(a) Nothing
(b) The size of A decreases and the size of B increases
(c) The size of A increases and the size of B decreases
(d) Both A and B will decrease in size
(e) Both A and B will increase in size.The excess pressure inside the smaller bubble A is greater and hence air from it will rush to B through the tube. The size of A will decrease further while the size of B will increase. The correct option therefore is (b).
You should note that the pressure on the concave side of a liquid surface is always greater by 2T/r. Consider the following question:
A tall metallic jar has a small hole of radius 0.07mm at its bottom. What is the approximate depth up to which the jar can be lowered vertically in water before any water penetrates in to it through the hole? (Surface tension of water = 0.073N/m)
(a) 7cm
(b) 11cm
(c) 16cm
(d) 21cm
(e) 27cmWater will begin to enter the jar through the hole when the hydrostatic pressure exceeds the allowed excess pressure of 2T/r on the concave side of the water surface at the hole. Therefore, the depth ‘h’ up to which the jar can be lowered safely is given by
hdg = 2T/r so that h = 2T/dgr = 2×0.073/(1000×9.8×0.00007) = 0.21m =21cm.
If T is the surface tension of soap solution, the amount of work done in increasing the radius of a soap bubble from r to 2r is
(a) (64πr2)T
(b) (32πr2)T
(c) (24πr2)T
(d) (16πr2)T
(e) (8πr2)T
(a) On the surface of Jupiter, height will be less than h.
(b) In a lift moving up with constant acceleration, height is less than h.
(c) On the surface of moon, height is more than h.
(d) In a lift moving down with constant acceleration, height is less than h.
(e) At the poles, height is less than that at equatorThe expression for surface tension (T) in terms of capillary rise in a capillary tube is
T = hrdg/2cosθ where ‘h’ is the capillary rise (or fall), ‘r’ is the radius of the tube, ‘d’ is the density of the liquid, ‘g’ is the acceleration due to gravity and ‘θ’ is the angle of contact. When ‘g’ is less, the capillary rise ‘h’ is more and vice versa. The value of ‘g’ is smaller in options (c) and (d) only so that the value of ‘h’ is greater in these two cases. So, option (d) is false. [Note that when a lift moves down with acceleration ‘a’, the effective value of acceleration due to gravity is (g-a)]