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Surface Tension and Capillary Action: Problems and Solutions, Study Guides, Projects, Research of Physics

irodov_problems_in_general_physics_2011

Typology: Study Guides, Projects, Research

2010/2011

Uploaded on 01/07/2023

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2.162. A vessel filled with air under pressure P
o
contains a soap
bubble of diameter
d.
The air pressure having been reduced isother-
mally n-fold, the bubble diameter increased mfold. Find the surface
tension of the soap water solution.
2.163. Find the pressure in an air bubble of diameter
d =
4.0 pm,
located in water at a depth
h =
5.0 m. The atmospheric pressure
has the standard value P
o
.
2.164. The diameter of a gas bubble formed at the bottom of a pond
is
d =
4.0 1.tm. When the bubble rises to the surface its diameter
increases n = 1.1 times. Find how deep is the pond at that spot.
The atmospheric pressure is standard, the gas expansion is assumed
to be isothermal.
2.165. Find the difference in height of mercury columns in two
communicating vertical capillaries whose diameters are
= 0.50 mm and
d
2
=
1.00 mm, if the contact angle 0 = 138°.
2.166. A vertical capillary with inside diameter 0.50 mm is
submerged into water so that the length of its part protruding over
the water surface is equal to
h =
25 mm. Find the curvature radius
of the meniscus.
2.167. A glass capillary of length
1 =
110 mm and inside dia-
meter
d =
20 pAn is submerged vertically into water. The upper end
of the capillary is sealed. The outside pressure is standard. To what
length
x
has the capillary to be submorged to make the water levels
inside and outside the capillary coincide?
2.168. When a vertical capillary of length
1
with the sealed upper
end was brought in contact with the surface of a liquid, the level
of this liquid rose to the height
h.
The liquid density is p, the inside
diameter of the capillary is
d,
the contact angle is 0, the atmospheric
pressure is P
o
. Find the surface tension of the liquid.
2.169. A glass rod of diameter d
1
= 1.5 mm is inserted sym-
metrically into a glass capillary with inside diameter
d
2
=
2.0 mm.
Then the whole arrangement is vertically oriented and brought in
contact with the surface of water. To what height will the water rise
in the capillary?
2.170. Two vertical plates submerged partially in a wetting liquid
form a wedge with a very small angle 6cp. The edge of this wedge is
vertical. The density of the liquid is p, its surface tension is a, the
contact angle is 0. Find the height
h,
to which the liquid rises, as a
function of the distance
x
from the edge.
2.171. A vertical water jet flows out of a round hole. One of the
horizontal sections of the jet has the diameter
d =
2 0 mm while
the other section located / = 20 mm lower has the diameter which
is n = 1.5 times less. Find the volume of the water flowing from
the hole each second.
2.172. A water drop falls in air with a uniform velocity. Find
the difference between the curvature radii of the drop's surface at
the upper and lower points of the drop separated by the distance
h =
2.3 mm.
94
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2.162. A vessel filled with air under pressure Pocontains a soap bubble of diameter d. The air pressure having been reduced isother- mally n-fold, the bubble diameter increased mfold. Find the surface tension of the soap water solution. 2.163. Find the pressure in an air bubble of diameter d = 4.0 pm, located in water at a depth h = 5.0 m. The atmospheric pressure has the standard value P o. 2.164. The diameter of a gas bubble formed at the bottom of a pond is (^) d = 4.0 1.tm. When the bubble rises to the surface its diameter increases n = 1.1 times. Find how deep is the pond at that spot. The atmospheric pressure is standard, the gas expansion is assumed to be isothermal. 2.165. Find the difference in height of mercury columns in two communicating vertical capillaries whose diameters are = 0.50 mm and d 2 = 1.00 mm, if the contact angle 0 = 138°. 2.166. A vertical capillary with inside diameter 0.50 mm is submerged into water so that the length of its part protruding over the water surface is equal to h = 25 mm. Find the curvature radius of the meniscus. 2.167. A glass capillary of length 1 = 110 mm and inside dia- meter d = 20 pAn is submerged vertically into water. The upper end of the capillary is sealed. The outside pressure is standard. To what length x has the capillary to be submorged to make the water levels inside and outside the capillary coincide? 2.168. When a vertical capillary of length 1 with the sealed upper end was brought in contact with the surface of a liquid, the level of this liquid rose to the height h. The liquid density is p, the inside diameter of the capillary is (^) d, the contact angle is 0, the atmospheric pressure is Po. Find the surface tension of the liquid. 2.169. A glass rod of diameter d1= 1.5 mm is inserted sym- metrically into a glass capillary with inside diameter d 2 =^ 2.0 mm. Then the whole arrangement is vertically oriented and brought in contact with the surface of water. To what height will the water rise in the capillary? 2.170. Two vertical plates submerged partially in a wetting liquid form a wedge with a very small angle 6cp. The edge of this wedge is vertical. The density of the liquid is p, its surface tension is a, the contact angle is 0. Find the height h, to which the liquid rises, as a function of the distance x from the edge. 2.171. A vertical water jet flows out of a round hole. One of the horizontal sections of the jet has the diameter d = 2 0 mm while the other section located / = 20 mm lower has the diameter which is n = 1.5 times less. Find the volume of the water flowing from the hole each second. 2.172. A water drop falls in air with a uniform velocity. Find the difference between the curvature radii of the drop's surface at the upper and lower points of the drop separated by the distance h = 2.3 mm.

2.173. A mercury drop shaped as a round tablet of radius R and thickness h is located between two horizontal glass plates. Assum- ing that h <<R , find the mass m of a weight which has to be placed on the upper plate to diminish the distance between the plates n-times. The contact angle equals 0. Calculate m if R = 2.0 cm, h = 0.38 mm, n = 2.0, and 0 = 135°. 2.174. Find the attraction force between two parallel glass plates, separated by a distance h = 0.10 mm, after a water drop of mass m = 70 mg was introduced between them. The wetting is assumed to be complete. 2.175. Two glass discs of radius R = 5.0 cm were wetted with water and put together so that the thickness of the water layer be- tween them was h = 1.9 p.m. Assuming the wetting to he complete, find the force that has to be applied at right angles to the plates in order to pull them apart. 2.176. Two vertical parallel glass plates are partially submerged in water. The distance between the plates is d =^ 0.10 mm, and their width is 1 = 12 cm. Assuming that the water between the plates does not reach the upper edges of the plates and that the wetting is complete, find the force of their mutual attraction. 2.177. Find the lifetime of a soap bubble of radius R connected with the atmosphere through a capillary of length 1 and inside radius r. The surface tension is a, the viscosity coefficient of the gas is 11. 2.178. A vertical capillary is brought in contact with the water surface. What amount of heat is liberated while the water rises along the capillary? The wetting is assumed to be complete, the sur- face tension equals a. 2.179. Find the free energy of the surface layer of (a) a mercury droplet of diameter d = 1.4 mm; (b) a soap bubble of diameter d = 6.0 mm if the surface tension of the soap water solution is equal to a = 45 mN/m. 2.180. Find the increment of the free energy of the surface layer when two identical mercury droplets, each of diameter d = 1.5 mm, merge isothermally. 2.181. Find the work to be performed in order to blow a soap bubble of radius R if the outside air pressure is equal to^ p, and the surface tension of the soap water solution is equal to a. 2.182. A soap bubble of radius r is inflated with an ideal gas. The atmospheric pressure is po, the surface tension of the soap water solution is a. Find the difference between the molar heat capacity of the gas during its heating inside the bubble and the molar heat capacity of the gas under constant pressure, C — Cp. 2.183. Considering the Carnot cycle as applied to a liquid film, show that in an isothermal process the amount of heat required for the formation of a unit area of the surface layer is equal to (^) q = = —T•daldT, where daldT is the temperature derivative of the surface tension.

Assuming the saturated vapour to be an ideal gas find the increment of entropy and internal energy of the system. 2.190. Water of mass m = 20 g is enclosed in a thermally insulat- ed cylinder at the temperature of 0 °C under a weightless piston whose area is S = 410 cm2. The outside pressure is equal to standard atmospheric pressure. To what height will the piston rise when the water absorbs Q = 20.0 kJ of heat? 2.191. One gram of saturated water vapour is enclosed in a therm- ally insulated cylinder under a weightless piston. The outside pres- sure being standard, m = 1.0 g of water is introduced into the cyl- inder at a temperature to= 22 °C. Neglecting the heat capacity of the cylinder and the friction of the piston against the cylinder's walls, find the work performed by the force of the atmospheric pres- sure during the lowering of the piston. 2.192. If an additional pressure Ap of a saturated vapour over a convex spherical surface of a liquid is considerably less than the vapour pressure over a plane surface, then Ap (p c Ipi)2oar, where p c and Pt are the densities of the vapour and the liquid, a is the sur- face tension, and r is the radius of curvature of the surface. Using this formula, find the diameter of water droplets at which the satu- rated vapour pressure exceeds the vapour pressure over the plane surface by = 1.0% at a temperature t = 27 °C. The vapour is assumed to be an ideal gas. 2.193. Find the mass of all molecules leaving one square centi- metre of water surface per second into a saturated water vapour above it at a temperature t = 100 °C. It is assumed that i1 = 3.6% of all water vapour molecules falling on the water surface are retained in the liquid phase. 2.194. Find the pressure of saturated tungsten vapour at a tem- perature T = 2000 K if a tungsten filament is known to lose a mass = 1.2-10-13g/(s•cm2) from a unit area per unit time when evaporating into high vacuum at this temperature. 2.195. By what magnitude would the pressure exerted by water on the walls of the vessel have increased if the intermolecular attrac- tion forces had vanished? 2.196. Find the internal pressure piof a liquid if its density p and specific latent heat of vaporization q are known. The heat q is assumed to be equal to the work performed against the forces of the internal pressure, and the liquid obeys the Van der Waals equation. Calculate pi in water. 2.197. Demonstrate that Eqs. (2.6a) and (2.6b) are valid for a substance, obeying the Van der Waals equation, in critical state. Instruction. Make use of the fact that the critical state corresponds to the point of inflection in the isothermal curve p (V). 2.198. Calculate the Van der Waals constants for carbon dioxide

if its critical temperature T„ = 304 K and critical pressure pc,. =

= (^) 73 atm.

7-9451 97

Fig. 2.5.

2.199. Find the specific volume of benzene (C6H6) in critical state if its critical temperature T „ = 562 K and critical pressure p„ = (^) 47 atm. 2.200. Write the Van der Waals equation via the reduced para- meters n, v, and r, having taken the corresponding critical values for the units of pressure, volume, and temperature. Using the equa- tion obtained, find how many times the gas temperature exceeds its critical temperature if the gas pressure is 12 times as high as critical pressure, and the volume of gas is equal to half the critical volume. 2.201. Knowing the Van der Waals constants, find: (a) the maximum volume which water of mass m = 1.00 kg can occupy in liquid state; (b) the maximum pressure of the saturated water vapour. 2.202. Calculate the temperature and density of carbon dioxide in critical state, assuming the gas to be a Van der Waals one. 2.203. What fraction of the volume of a vessel must liquid ether occupy at room temperature in order to pass into critical state when critical temperature is reached? Ether

has T , = 467 K, per = 35.5 atm, p

M = 74 g/mol.

2.204. Demonstrate that the straight line 1-5^ corresponding to the isother- mal-isobaric phase transition cuts the Van der Waals isotherm so that areas I and II are equal (Fig. 2.5). 2.205. What fraction of water su- percooled down to the temperature t = —20 °C under standard pressure turns into ice when the system passes into the equilibrium state? At what temperature of the supercooled water does it turn into ice completely? 2.206. Find the increment of the ice melting temperature in the vicinity of 0 °C when the pressure is increased by Ap = 1.00 atm. The specific volume of ice exceeds that of water byiAV' = 0.091 cm3/g. 2.207. Find the specific volume of saturated water vapour under standard pressure if a decrease of pressure by Ap = 3.2 kPa is known to decrease the water boiling temperature by AT = 0.9 K. 2.208. Assuming the saturated water vapour to be ideal, find its pressure at the temperature 101.1 °C. 2.209. A small amount of water and its saturated vapour are en- closed in a vessel at a temperature t = 100^ °C. How much (in per cent) will the mass of the saturated vapour increase if the temperature of the system goes up by AT = 1.5 K? Assume that the vapour is an ideal gas and the specific volume of water is negligible as compared to that of vapour. 2.210. Find the pressure of saturated vapour as a function of temperature p (T) if at a temperature Toits pressure equals po.