Properties of Matter

JEE Physics · 167 questions · Page 4 of 17 · Click an option or "Show Solution" to reveal answer

Q31
Spherical balls of radius RR are falling in a viscous fluid of viscosity η\eta with a velocity v.v. The retarding viscous force acting on the spherical ball is
A inversely proportional to both radius RR and velocity vv
B directly proportional to both radius RR and velocity vv
C directly proportional to RR but inversely proportional to vv
D inversely proportional to R,R, but directly proportional to velocity vv
Correct Answer
Option B
Solution

From Stoke's law, viscous force acting on the ball falling into a viscous fluid

F=6πηRvF = 6\pi \eta Rv

\therefore

FRF \propto R

and

FvF \propto v

hence

FF

is directly proportional to radius & velocity.

Q32
If two soap bubbles of different radii are connected by a tube
A air flows from the smaller bubble to the bigger
B air flows from bigger bubble to the smaller bubble till the sizes are interchanged
C air flows from the bigger bubble to the smaller bubble till the sizes become equal
D there is no flow of air.
Correct Answer
Option A
Solution

Pressure inside the bubble, P

=p0+4TR= {p_0} + {{4T} \over R}

So

P1RP \propto {1 \over R}

where R is the radius of the bubble.

It means pressure inside a smaller bubble is greater than the inside of a bigger bubble.

So when two bubbles are connected by a tube, air will flow from smaller bubble to bigger bubble and the size of bigger bubble will increase.

Q33
If SS is stress and YY is young's modulus of material of a wire, the energy stored in the wire per unit volume is
A S22Y{{{S^2}} \over {2Y}}
B 2S2Y2{S^2}Y
C S2Y{S \over {2Y}}
D 2YS2{{2Y} \over {{S^2}}}
Correct Answer
Option A
Solution

Energy stored per unit volume of wire,

E=12×stress×strainE = {1 \over 2} \times \,stress\, \times \,strain

\therefore

E=12×stress×stressY=12S2YE = {1 \over 2} \times \,stress\, \times \,{{stress} \over Y} = {1 \over 2}{{{S^2}} \over Y}

[ As Young's modulus(Y) =

StressStrain{{Stress} \over {Strain}}

\therefore Strain =

StressY{{Stress} \over Y}

]

Q34
A 2020 cmcm long capillary tube is dipped in water. The water rises up to 88 cm.cm. If the entire arrangement is put in a freely falling elevator the length of water column in the capillary tube will be
A 1010 cmcm
B 88 cmcm
C 2020 cmcm
D 44 cmcm
Correct Answer
Option C
Solution

In freely falling elevator

gg

= 0 Water fills the tube entirely in gravity less condition.

Hence, length of water column in the capillary tube is 20 cm.

Q35
A spherical solid ball of volume VV is made of a material of density ρ1{\rho _1}. It is falling through a liquid of density ρ2(ρ2<ρ1){\rho _2}\left( {{\rho _2} < {\rho _1}} \right). Assume that the liquid applies a viscous force on the ball that is proportional to the square of its speed v,v, i.e., Fviscous=kv2(k>0).{F_{viscous}} = - k{v^2}\left( {k > 0} \right). The terminal speed of the ball is
A Vg(ρ1ρ2)k\sqrt {{{Vg\left( {{\rho _1} - {\rho _2}} \right)} \over k}}
B Vgρ1k{{{Vg{\rho _1}} \over k}}
C Vgρ1k\sqrt {{{Vg{\rho _1}} \over k}}
D Vg(ρ1ρ2)k{{Vg\left( {{\rho _1} - {\rho _2}} \right)} \over k}
Correct Answer
Option A
Solution

The forces acting on the ball - (1) mg =

Vρ1gV{\rho _1}g

downward direction (2) Thrust upward direction ( By Archimedes principle ) (3) Force of friction ( Buoynat force) upward direction The ball reaches to its terminal speed

(vt)\left( {{v_t}} \right)

when acceleration = 0. So, weight == Buoyant force ++ Viscous force \therefore

Vρ1g=Vρ2g+kvt2V\rho {}_1g = V{\rho _2}g + kv_t^2

\therefore

vt=Vg(ρ1ρ2)k{v_t} = \sqrt {{{Vg\left( {{\rho _1} - {\rho _2}} \right)} \over k}}
Q36
Two wires are made of the same material and have the same volume. However wire 11 has cross-sectional area AA and wire 22 has cross-sectional area 3A.3A. If the length of wire 11 increases by Δx\Delta x on applying force F,F, how much force is needed to stretch wire 22 by the same amount?
A 4F4F
B 6F6F
C 9F9F
D FF
Correct Answer
Option C
Solution

As shown in the figure, the wires will have the same Young's modulus (same material) and the length of the wire of area of cross-section

3A3A

will be

/3\ell /3

(same volume as wire

11

). For wire

1,1,
y=F/AΔx/...(i)y = {{F/A} \over {\Delta x/\ell }}\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,...(i)

For wire

2.2.
Y=F/3AΔx/(/3)........(ii)Y = {{F'/3A} \over {\Delta x/\left( {\ell /3} \right)}}........(ii)

From

(i)(i)

and

(ii),(ii),
FA×Δx=F3A×3ΔxF=9F{F \over A} \times {\ell \over {\Delta x}} = {{F'} \over {3A}} \times {\ell \over {3\Delta x}} \Rightarrow F' = 9F
Q37
Water is flowing continuously from a tap having an internal diameter 8×103m.8 \times {10^{ - 3}}\,\,m. The water velocity as it leaves the tap is 0.4ms10.4\,\,m{s^{ - 1}} . The diameter of the water stream at a distance 2×101m2 \times {10^{ - 1}}\,\,m below the tap is close to :
A 7.5×103m7.5 \times {10^{ - 3}}m
B 9.6×103m9.6 \times {10^{ - 3}}m
C 3.6×103m3.6 \times {10^{ - 3}}m
D 5.0×103m5.0 \times {10^{ - 3}}m
Correct Answer
Option C
Solution

From Bernoulli's theorem,

P0+12ρv12ρgh=P0+12ρv22+0{P_0} + {1 \over 2}\rho v_1^2\rho gh = {P_0} + {1 \over 2}\rho v_2^2 + 0
v2=v12+2gh{v_2} = \sqrt {v_1^2 + 2gh}
=0.16+2×10×0.2= \sqrt {0.16 + 2 \times 10 \times 0.2}
=2.03m/s= 2.03\,m/s

From equation of continuity

A2v2=A1v1{A_2}{v_2} = {A_1}{v_1}
πD224×v2=πD124v1\pi {{D_2^2} \over 4} \times {v_2} = \pi {{D_1^2} \over 4}{v_1}
D1=D2v1v2=3.55×103m\Rightarrow \,\,{D_1} = {D_2}\sqrt {{{{v_1}} \over {{v_2}}}} = 3.55 \times {10^{ - 3}}m
Q38
A uniform cylinder of length LL and mass MM having cross-sectional area AA is suspended, with its length vertical, from a fixed point by a mass-less spring such that it is half submerged in a liquid of density σ\sigma at equilibrium position. The extension x0{x_0} of the spring when it is in equilibrium is:
A Mgk{{Mg} \over k}
B Mgk(1LAσM){{Mg} \over k}\left( {1 - {{LA\sigma } \over M}} \right)
C Mgk(1LAσ2M){{Mg} \over k}\left( {1 - {{LA\sigma } \over {2M}}} \right)
D Mgk(1+LAσM){{Mg} \over k}\left( {1 + {{LA\sigma } \over M}} \right)
Correct Answer
Option C
Solution

From figure,

kx0+FB=Mgk{x_0} + {F_B} = Mg
kx0+σL2Ag=Mgk{x_0} + \sigma {L \over 2}Ag = Mg

[ as mass == density ×\times volume ]

kx0=MgσL2Ag\Rightarrow k{x_0} = Mg - \sigma {L \over 2}Ag
x0=MgσLAg2k\Rightarrow {x_0} = {{Mg - {{\sigma LAg} \over 2}} \over k}
=Mgk(1LAσ2M)= {{Mg} \over k}\left( {1 - {{LA\sigma } \over {2M}}} \right)
Q39
The pressure that has to be applied to the ends of a steel wire of length 1010 cmcm to keep its length constant when its temperature is raised by 100C{100^ \circ }C is: (For steel Young's modulus is 2×1011Nm22 \times {10^{11}}\,\,N{m^{ - 2}} and coefficient of thermal expansion is 1.1×105K11.1 \times {10^{ - 5}}\,{K^{ - 1}} )
A 2.2×108Pa2.2 \times {10^8}\,\,Pa
B 2.2×109Pa2.2 \times {10^9}\,\,Pa
C 2.2×107Pa2.2 \times {10^7}\,\,Pa
D 2.2×106Pa2.2 \times {10^6}\,\,Pa
Correct Answer
Option A
Solution

Young's modulus

Y=stressstrainY = {{stress} \over {strain}}
stress=Y×strainstress = Y \times strain
StressStress

in steel wire == Applied

pressurepressure
PressurePressure

==

stressstress

==

Y×strainY \times \,strain
Strain=ΔLL=αΔTStrain = {{\Delta L} \over L} = \alpha \Delta T

(As length is constant)

=2×1011×1.1×105×100= 2 \times {10^{11}} \times 1.1 \times {10^{ - 5}} \times 100
=2.2×108Pa= 2.2 \times {10^8}Pa
Q40
An open glass tube is immersed in mercury in such a way that a length of 88 cmcm extends above the mercury level. The open end of the tube is then closed and scaled and the tube is raised vertically up by additional 4646 cmcm. What will be length of the air column above mercury in the tube now? (Atmospheric pressure =76=76 cmcm of HgHg)
A 1616 cmcm
B 2222 cmcm
C 3838 cmcm
D 66 cmcm
Correct Answer
Option A
Solution

Length of the air column above mercury in the tube is,

P+x=P0P + x = {P_0}
P=(76x)\Rightarrow P = \left( {76 - x} \right)
8×A×76=(76x)×A×(54x)\Rightarrow 8 \times A \times 76 = \left( {76 - x} \right) \times A \times \left( {54 - x} \right)

\therefore

x=38x=38

Thus, length of air column

=5438=16cm.=54-38=16cm.
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