Properties of Matter

NEET Physics · 97 questions · Page 3 of 10 · Click an option or "Show Solution" to reveal answer

Q21
The unit of thermal conductivity is :
A J m –1 K –1
B W m K –1
C J m K –1
D W m –1 K –1
Correct Answer
Option D
Solution

We know, Heat transfer (Q) = KA

(ΔTΔx)\left( {{{\Delta T} \over {\Delta x}}} \right)

×\timest Here, K is the coefficient of thermal conductivity J = (K)m 2

kelvinm{{kelvin} \over m}

×\times s \therefore Unit of K = Wm –1 K –1

Q22
When a block of mass M is suspended by a long wire of length L, the length of the wire becomes (L + ll). The elastic potential energy stored in the extended wire is :
A Mgl
B mgL
C 12{1 \over 2}Mgl
D 12{1 \over 2}MgL
Correct Answer
Option C
Solution

Elastic potential energy U =

12{1 \over 2}

(work done due to gravity) =

12{1 \over 2}

Mgl

Q23
A soap bubble, having radius of 1 mm, is blown from a detergent solution having a surface tension of 2.5 × \times 10 –2 N/m. The pressure inside the bubble equals at a point Z 0 below the free surface of water in a container. Taking g = 10 m/s 2 , density of water = 10 3 kg/m 3 , the value of Z 0 is :
A 1 cm
B 10 cm
C 100 cm
D 0.5 cm
Correct Answer
Option A
Solution

P = P 0 + ρ\rhogZ 0 .........(i) Also, P = P 0 +

4TR{{4T} \over R}

.....(ii) From (i) and (ii), ρ\rhogZ 0 =

4TR{{4T} \over R}

\therefore Z 0 =

4TρgR{{4T} \over {\rho gR}}

=

4×2.5×102103×10×103{{4 \times 2.5 \times {{10}^{ - 2}}} \over {{{10}^3} \times 10 \times {{10}^{ - 3}}}}

= 10 -2 m = 1 cm

Q24
A copper rod of 88 cm and an aluminium rod of unknown length have their increase in length independent of increase in tmperature. The length of aluminium rod is : (α\alpha Cu = 1.7 × 10 –5 K –1 and α\alpha Al = 2.2 × 10 –5 K –1 )
A 119.9 cm
B 88 cm
C 68 cm
D 6.8 cm
Correct Answer
Option C
Solution

At any temperature

(Δl)Cu=(Δl)Al{\left( {\Delta l} \right)_{Cu}} = {\left( {\Delta l} \right)_{Al}}
lCuαCuΔT=lAlαAlΔT{l_{Cu}}{\alpha _{Cu}}\Delta T = {l_{Al}}{\alpha _{Al}}\Delta T

\Rightarrow 88 ×\times 1.7 ×\times 10 -5 =

lAl{l_{Al}}

×\times 2.2 × 10 –5 \Rightarrow

lAl{l_{Al}}

= 68 cm

Q25
A small hole of area of cross-section 2 mm 2 present near the bottom of a fully filled open tank of height 2 m. Taking g = 10 m/s 2 , the rate of flow of water through the open hole would be nearly :
A 8.9 × 10 –6 m 3 /s
B 2.23 × 10 –6 m 3 /s
C 6.4 × 10 –6 m 3 /s
D 12.6 × 10 –6 m 3 /s
Correct Answer
Option D
Solution

volume flow rate = Av = A

2gh\sqrt {2gh}

= 2 ×\times 10 -6 ×\times

2×10×2\sqrt {2 \times 10 \times 2}

= 2 ×\times 2 ×\times 3.14 ×\times 10 -6 m 3 /s = 12.56 ×\times 10 -6 m 3 /s = 12.6 ×\times 10 -6 m 3 /s

Q26
Two wires are made of the same material and have the same volume. The first wire has cross-sectional area A and the second wire has cross-sectional area 3A. If the length of the first wire is increased by Δ\Delta l on applying a force F, how much force is needed to stretch the second wire by the same amount?
A 6F
B F
C 9F
D 4F
Correct Answer
Option C
Solution

Let the wire 1 is of length = l and wire 2 of length =

l3{l \over 3}

Now area of wire 1 = A while area of wire 2 = 3A For wire 1,

Δ\Delta

l =

(FAY)l\left( {{F \over {AY}}} \right)l

....(i) For wire 2, let F' force is applied

Δ\Delta

l =

(F3AY)l3\left( {{{F'} \over {3AY}}} \right){l \over 3}

....(2) From equation (i) & (ii)

(FAY)l\left( {{F \over {AY}}} \right)l

=

(F3AY)l3\left( {{{F'} \over {3AY}}} \right){l \over 3}

\Rightarrow F' = 9F

Q27
The power radiated by a black body is P and it radiates maximum energy at wavelength, λ\lambda 0 . If the temperature of the black body is now changed so that it radiates maximum energy at wavelength 34λ0{3 \over 4}{\lambda _0}, the power radiated by it becomes nP. The value of n is
A 34{3 \over 4}
B 43{4 \over 3}
C 25681{{256} \over {81}}
D 81256{{81} \over {256}}
Correct Answer
Option C
Solution

From Wien's law, λ\lambda max T = constant \therefore λ\lambda max 1 T 1 = λ\lambda max 2 T 2 \Rightarrow λ\lambda 0 T 1 =

3λ04{{3{\lambda _0}} \over 4}

T 2 \Rightarrow

T2T1=43{{T_2} \over T_1} = {4 \over 3}

According to Stefan-Boltzmann law, energy emitted unit time by a black body is Aeσ\sigmaT 4 , \therefore P \propto T 4 So

P2P1=(T2T1)4{{{P_2}} \over {{P_1}}} = {\left( {{{{T_2}} \over {{T_1}}}} \right)^4}

=

(43)4{\left( {{4 \over 3}} \right)^4}

Here, P 2 = nP and P 1 = P So,

nPP=n=(T2T1)4=(43)4=25681{{nP} \over P} = n = {\left( {{{{T_2}} \over {{T_1}}}} \right)^4} = {\left( {{4 \over 3}} \right)^4} = {{256} \over {81}}
Q28
A small sphere of radius ‘r’ falls from rest in a viscous liquid. As a result, heat is produced due to viscous force. The rate of production of heat when the sphere attains its terminal velocity, is proportional to
A r 3
B r 2
C r 5
D r 4
Correct Answer
Option C
Solution

Power = rate of production of heat = F.V = 6π\piη\etarV T .

V T = = 6π\piη\etarV T 2 [ As F = 6π\piη\etarV T from stoke’s formula ] \because Terminal velocity V T =

2r2(ρσ)g9η{{2{r^2}\left( {\rho - \sigma } \right)g} \over {9\eta }}

\therefore V T \propto r 2 \therefore Power \propto 6π\piη\etar

[4r4(ρσ)2g281η2]\left[ {{{4{r^4}{{\left( {\rho - \sigma } \right)}^2}{g^2}} \over {81{\eta ^2}}}} \right]

\Rightarrow Power \propto r 5

Q29
Two rods A and B of different materials are welded together as shown in figure. Their thermal conductivities are K 1 and K 2 . The thermal conductivity of the composite will be
A 3(K1+K2)2{{3\left( {{K_1} + {K_2}} \right)} \over 2}
B K1+K2{K_1} + {K_2}
C 2(K1+K2)2\left( {{K_1} + {K_2}} \right)
D K1+K22{{{K_1} + {K_2}} \over 2}
Correct Answer
Option D
Solution

Equivalent thermal conductivity of the composite rod in parallel combination will be,

K=K1A1+K2A2A1+A2=K1+K22K = {{{K_1}{A_1} + {K_2}{A_2}} \over {{A_1} + {A_2}}} = {{{K_1} + {K_2}} \over 2}
Q30
The bulk modulus of a spherical object is 'B'. If it is subjected to uniform pressure 'P', the fractional decrease in radius is
A B3p{B \over {3p}}
B 3pB{{3p} \over B}
C p3B{p \over {3B}}
D pB{p \over B}
Correct Answer
Option C
Solution

Bulk modulus is given by

B=P(ΔVV)ΔVV=PBB = {P \over {\left( {{{\Delta V} \over V}} \right)}} \Rightarrow {{\Delta V} \over V} = {P \over B}
3ΔRR=PB3{{\Delta R} \over R} = {P \over B}

(here,

ΔRR{{\Delta R} \over R}

= fractional decreases in radius)

ΔRR=P3B\Rightarrow {{\Delta R} \over R} = {P \over {3B}}
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