Mechanical Properties Of Fluids

Sponsor Area

Question
CBSEENPH11020579

A certain number of spherical drops of a liquid of radius r coalesce to form a single drop of radius R and volume V. If T is the surface tension of the liquid, then

  • Energy = 4VT open parentheses 1 over straight r minus 1 over straight R close parentheses is released.

  • Energy = 3VTopen parentheses 1 over straight r plus 1 over R close parentheses is absorbed

  • Energy = 3 VT open parentheses 1 over straight r minus 1 over straight R close parentheses is released

  • Energy is neither absorbed nor released.

Solution

C.

Energy = 3 VT open parentheses 1 over straight r minus 1 over straight R close parentheses is released

If the surface area changes, it will change the surface energy also.
When the surface area decreases, it means energy is released ad vice-versa.
Change in surface energy is increment straight A space straight x space straight T   ... (i)
Let, there be n number of drops initially.
So, increment straight A space equals space 4 πR squared space minus space straight n space left parenthesis 4 πr squared right parenthesis       ... (ii)
Volume is constant.
So, straight n space 4 over 3 πr cubed space equals space 4 over 3 πr cubed space equals space straight V         ... (iii)
From equations (ii) and (iii), we have
WiredFaculty
Since, R > r, incrementA is negative.
That is, the surface area is decreased.
Hence, energy must be released.
Energy released = increment straight A space straight x space straight T space equals space minus 3 VT open parentheses 1 over straight r minus 1 over straight R close parentheses
In the above expression, (-)ve sign shows that amount of energy is released.

Sponsor Area

Question
CBSEENPH11020810

A U tube with both ends open to the atmosphere is partially filled with water. Oil, which is immiscible with water, is poured into one side until it stands at a distance of 10 mm above the water level on the other side. Meanwhile, the water rises by 65 mm from its original level (see diagram). The density of the oil is
WiredFaculty

  • 650 kg m–3

  • 425 kg m–3

  • 800 kg m–3

  • 928 kg m–3

Solution

D.

928 kg m–3

hoil ρoil g = hwater ρwater g
140 × ρoil= 130 × ρwater
WiredFaculty

Question
CBSEENPH11020643

If dimensions of critical velocity vc of a liquid flowing through  a tube are expressed as left square bracket straight eta to the power of straight x space straight rho to the power of straight y space straight r to the power of straight z right square bracket comma space where space straight eta comma space straight rho space and space straight r are the coefficient of viscosity of liquid, density of liquid and radius of the tube respectively, then the values of x, y and z are given by

  • 1,-1,-1

  • -1,-1,1

  • -1,-1,-1

  • 1,1,1

Solution

A.

1,-1,-1

According to the principle of homogeneity of dimension states that, a physical quantity equation will be dimensionally correct if the dimension of all the terms occurring on both sides of the equations is same.
Given critical velocity of liquid flowing through a tube are expressed as
WiredFaculty
x+ y = 0, - x-3y+z = 1, -x = -1
z = -11 x = 1, y = -1

Question
CBSEENPH11020612

The wettability of a surface by a liquid depends primarily on

  • viscosity

  • surface tension

  • density

  • angle of contact between the surface and the liquid

Solution

D.

angle of contact between the surface and the liquid

The value of angle of contact determines whether a liquid will spread on the surface or not.

Question
CBSEENPH12039767

The wind with speed 40 m/s blows parallel to the roof of a house. The area of the roof is 250m2. Assuming that the pressure inside the house is atmospheric pressure, the force exerted by the wind on the roof and the direction of the force will be( pair = 1.2 kg/m3)

  • 4.8 x 105 N, downwards

  • 4.8 x105 N , upwards

  • 2.4 x 105 N , upwards

  • 2.4 x 105 N , upwards

Solution

C.

2.4 x 105 N , upwards

From Bernoulli's theorem
straight p subscript 1 space plus 1 half ρv subscript 1 superscript 2 space equals space straight p subscript 2 plus 1 half ρv subscript 2 superscript 2
Where p1,p2 are pressure inside and outside the roof and v1, v2 are velocities of the wind inside and outside the roof. Neglect the Width of the roof.
Pressure difference is 
p1 -p2 =WiredFaculty
Force acting on the roof is given by
F= (p1 -p2) A = 960 x 250
 = 24 x 104 N  = 24 x 105 N
As the pressure inside the roof is more than outside to it. So the force will act in the upward direction i.e. F = 24 x 105 N -upward.

3