Properties of Matter

JEE Physics · 167 questions · Page 1 of 17 · Click an option or "Show Solution" to reveal answer

Q1
The height of liquid column raised in a capillary tube of certain radius when dipped in liquid A vertically is, 5 cm5 \mathrm{~cm}. If the tube is dipped in a similar manner in another liquid B\mathrm{B} of surface tension and density double the values of liquid A\mathrm{A}, the height of liquid column raised in liquid B\mathrm{B} would be __________ m.
A 0.05
B 0.20
C 0.5
D 0.10
Correct Answer
Option A
Solution

height of capillary rise

=2scosθρgR= {{2s\cos \theta } \over {\rho gR}}

When in A 5 cm

=2sAcosθρAgR= {{2{s_A}\cos \theta } \over {{\rho _A}gR}}

When in B

h=2sBcosθρBgRh = {{2{s_B}\cos \theta } \over {{\rho _B}gR}}
sB=2sA{s_B} = 2{s_A}

and

ρB=2ρA{\rho _B} = 2{\rho _A}
h=2×2sA×cosθ2ρAgR=5h = {{2 \times 2{s_A} \times \cos \theta } \over {2{\rho _A}gR}} = 5

cm

Q2
A solid steel ball of diameter 3.6 mm acquired terminal velocity 2.45×102 m/s2.45 \times 10^{-2} \mathrm{~m} / \mathrm{s} while falling under gravity through an oil of density 925 kg m3925 \mathrm{~kg} \mathrm{~m}^{-3}. Take density of steel as 7825 kg m37825 \mathrm{~kg} \mathrm{~m}^{-3} and g as 9.8 m/s29.8 \mathrm{~m} / \mathrm{s}^2. The viscosity of the oil in SI unit is
A 2.18
B 1.68
C 2.38
D 1.99
Correct Answer
Option D
Solution

To determine the viscosity of the oil, we use the formula for the terminal velocity of a sphere falling through a viscous fluid: vT=29(ρsρf)r2gη v_T = \dfrac{2}{9} \dfrac{(\rho_s - \rho_f) r^2 g}{\eta} Where: vT v_T is the terminal velocity, ρs \rho_s is the density of the steel ball, ρf \rho_f is the density of the fluid, r r is the radius of the ball, g g is the acceleration due to gravity, η \eta is the viscosity of the fluid.

Given: Diameter of the steel ball = 3.6 mm, therefore radius r=1.8 r = 1.8 mm = 1.8×103 1.8 \times 10^{-3} m, Terminal velocity vT=2.45×102 v_T = 2.45 \times 10^{-2} m/s, Density of oil ρf=925 \rho_f = 925 kg/m3^3, Density of steel ρs=7825 \rho_s = 7825 kg/m3^3, Acceleration due to gravity g=9.8 g = 9.8 m/s2^2.

Rearranging the formula to solve for η\eta: η=29(ρsρf)r2gvT \eta = \dfrac{2}{9} \cdot \dfrac{(\rho_s - \rho_f) \cdot r^2 \cdot g}{v_T} Substituting the known values into the equation: η=29(7825925)(1.8×103)29.82.45×102 \eta = \dfrac{2}{9} \cdot \dfrac{(7825 - 925) \cdot (1.8 \times 10^{-3})^2 \cdot 9.8}{2.45 \times 10^{-2}} Calculating this, we approximate the viscosity η\eta to be: η1.99Pas \eta \approx 1.99 \, \text{Pa}\cdot\text{s} Thus, the viscosity of the oil is approximately 1.99 Pa·s.

Q3
Given below are two statements : One is labelled as Assertion (A) and the other is labelled as Reason (R). Assertion (A): Clothes containing oil or grease stains cannot be cleaned by water wash. Reason (R): Because the angle of contact between the oil/grease and water is obtuse. In the light of the above statements, choose the correct answer from the option given below.
A Both (A) and (R) are true and (R) is the correct explanation of (A)
B Both (A) and (R) are true but (R) is not the correct explanation of (A)
C (A) is true but (R) is false
D (A) is false but (R) is true
Correct Answer
Option A
Solution

Due to obtuse angle of contact the water doesn't wet the oiled surface properly and cannot wash it also.

\Rightarrow Assertion is correct and Reason given is a correct explanation.

Q4
Under the same load, wire A having length 5.0 m5.0 \mathrm{~m} and cross section 2.5×105 m22.5 \times 10^{-5} \mathrm{~m}^{2} stretches uniformly by the same amount as another wire B of length 6.0 m6.0 \mathrm{~m} and a cross section of 3.0×1053.0 \times 10^{-5} m2\mathrm{m}^{2} stretches. The ratio of the Young's modulus of wire A to that of wire BB will be :
A 1:21: 2
B 1:41: 4
C 1:11: 1
D 1:101: 10
Correct Answer
Option C
Solution

Δ=FSY\Delta \ell=\dfrac{F \ell}{S Y} FF is same for both wire and Δ\Delta \ell is also same

ΔF=SYASAYA=BSBYB52.5×YA=63×YBYAYB=1\begin{aligned} & \frac{\Delta \ell}{F}=\frac{\ell}{S Y} \\\\ & \Rightarrow \frac{\ell_{A}}{S_{A} Y_{A}}=\frac{\ell_{B}}{S_{B} Y_{B}} \\\\ & \Rightarrow \frac{5}{2.5 \times Y_{A}}=\frac{6}{3 \times Y_{B}} \\\\ & \Rightarrow \frac{Y_{A}}{Y_{B}}=1 \end{aligned}
Q5
Water flows into a large tank with flat bottom at the rate of 10–4m3s–1. Water is also leaking out of a hole ofarea 1 cm2 at its bottom. If the height of the water in the tank remains steady, then this height is -
A 2.9 cm
B 5.1 cm
C 4 cm
D 1.7 cm
Correct Answer
Option B
Solution

Since height of water column is constant therefore, water inflow rate (Qin) = water outflow rate Qin = 10-4 m3s-1 Qout = Au = 10-4 ×\times

2gh\sqrt {2gh}

10-4 = 10-4

20×h\sqrt {20 \times h}

h =

120m{1 \over {20}}m

h = 5cm

Q6
A air bubble of radius 1 cm in water has an upward acceleration 9.8 cm s–2. The density of water is 1 gm cm–3 and water offers negligible drag force on the bubble. The mass of the bubble is (g = 980 cm/s2).
A 1.52 gm
B 4.51 gm
C 3.15 gm
D 4.15 gm
Correct Answer
Option D
Solution

B - mg = ma \Rightarrow m =

Bg+a{B \over {g + a}}

=

Vρwgg+a{{V{\rho _w}g} \over {g + a}}

=

Vρw1+ag{{V{\rho _w}} \over {1 + {a \over g}}}

=

43π(1)3×11+9.8980{{{4 \over 3}\pi {{\left( 1 \right)}^3} \times 1} \over {1 + {{9.8} \over {980}}}}

= 4.15 gm

Q7
The normal density of a material is ρ\rho and its bulk modulus of elasticity is K. The magnitude of increase in density of material, when a pressure P is applied uniformly on all sides, will be :
A ρKP{{\rho K} \over P}
B PKρ{{PK} \over \rho }
C ρPK{{\rho P} \over K}
D KρP{K \over {\rho P}}
Correct Answer
Option C
Solution

Bulk modulus

K=ΔPΔvv=ΔPvΔvK = {{ - \Delta P} \over {{{\Delta v} \over v}}} = {{ - \Delta Pv} \over {\Delta v}}

We know,

ρ=MV\rho = {M \over V}

So,

Δρρ=Δvv{{ - \Delta \rho } \over \rho } = {{\Delta v} \over v}
K=ΔP(Δρρ)=ρΔPΔρK = {{ - \Delta P} \over {\left( { - {{\Delta \rho } \over \rho }} \right)}} = {{\rho \Delta P} \over {\Delta \rho }}
Δρ=ρΔPK\Delta \rho = {{\rho \Delta P} \over K}
Δρ=ρPK\Delta \rho = {{\rho P} \over K}
Q8
The terminal velocity (vt) of the spherical rain drop depends on the radius (r) of the spherical rain drop as :
A r1/2
B r
C r2
D r3
Correct Answer
Option C
Solution
6πηvtr=43πr3(ρσ)g6\pi \eta {v_t}r = {4 \over 3}\pi {r^3}(\rho - \sigma )g
vt=Cr2\Rightarrow {v_t} = C{r^2}

where C is a constant or

vtr2{v_t} \propto {r^2}
Q9
A balloon has mass of 10 g10 \mathrm{~g} in air. The air escapes from the balloon at a uniform rate with velocity 4.5 cm/s4.5 \mathrm{~cm} / \mathrm{s}. If the balloon shrinks in 5 s5 \mathrm{~s} completely. Then, the average force acting on that balloon will be (in dyne).
A 3
B 9
C 12
D 18
Correct Answer
Option B
Solution
Favg=μ×vrel{F_{avg}} = \mu \times {v_{rel}}
=105×4.5=9= {{10} \over 5} \times 4.5 = 9
Q10
For a solid rod, the Young's modulus of elasticity is 3.2×1011Nm23.2 \times 10^{11} \mathrm{Nm}^{-2} and density is 8×103 kg m38 \times 10^3 \mathrm{~kg} \mathrm{~m}^{-3}. The velocity of longitudinal wave in the rod will be.
A 3.65×103 ms13.65 \times 10^3 \mathrm{~ms}^{-1}
B 6.32×103 ms16.32 \times 10^3 \mathrm{~ms}^{-1}
C 18.96×103 ms118.96 \times 10^3 \mathrm{~ms}^{-1}
D 145.75×103 ms1145.75 \times 10^3 \mathrm{~ms}^{-1}
Correct Answer
Option B
Solution

v=Yρ=3.2×10118×103v=\sqrt{\dfrac{Y}{\rho}}=\sqrt{\dfrac{3.2 \times 10^{11}}{8 \times 10^{3}}}

=0.4×108=40×106=6.32×103 m/s\begin{aligned} & =\sqrt {0.4 \times {{10}^8}} \\\\ & = \sqrt {40 \times {{10}^6}} \\\\ & =6.32 \times 10^{3} \mathrm{~m} / \mathrm{s} \end{aligned}
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