Units & Measurements

NEET Physics · 152 questions · Page 14 of 16 · Click an option or "Show Solution" to reveal answer

Q131
Planck's constant (h), speed of light in vacuum (c) and Newton's gravitional constant (G) are three fundamental constants. Which of the following combinations of these has the dimension of length ?
A hGc3/2{{\sqrt {hG} } \over {{c^{3/2}}}}
B hGc5/2{{\sqrt {hG} } \over {{c^{5/2}}}}
C hcG\sqrt {{{hc} \over G}}
D Gch3/2\sqrt {{{Gc} \over {{h^{3/2}}}}}
Correct Answer
Option A
Solution

According to question, L \propto h p c q G r [M 0 LT 0 ] = [ML 2 T -1 ] p [LT -1 ] q [M -1 L 3 T -2 ] r Equating power both sides, we get p - r = 0 ......(1) 2p + q + 3r = 1 ......(2) - p - q - 2r = 0 ......(

3) Solving equation (1), (2), (3), we get p = r =

12{1 \over 2}

, q =

32- {3 \over 2}

\therefore L =

hGc3/2{{\sqrt {hG} } \over {{c^{3/2}}}}
Q132
If dimensions of critical velocity υ\upsilon c of a liquid flowing through a tube are expressed as [ηxρyrz]\left[ {{\eta ^x}{\rho ^y}{r^z}} \right] where η,ρ\eta ,\rho and 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
A -1, -1, -1
B 1, 1, 1
C 1, -1, -1
D -1, -1, 1
Correct Answer
Option C
Solution
υ\upsilon

c =

[ηxρyrz]\left[ {{\eta ^x}{\rho ^y}{r^z}} \right]

Put dimensions of various quantities, [M 0 LT -1 ] = [ML -1 T -1 ] x [ML -3 T 0 ] y [M 0 LT 0 ] z = [M x + y L - x - 3y + z T - x ] Equating power both sides, we get x + y = 0; - x - 3y + z = 1; - x = - 1 On solving, we get x = 1, y = -1, z = -1

Q133
If energy (E), velocity (V) and time (T) are chosen as the fundamental quantities, the dimensional formula of surface tension will be
A [EV2T2]\left[ {E{V^{ - 2}}{T^{ - 2}}} \right]
B [E2V1T3]\left[ {{E^{ - 2}}{V^{ - 1}}{T^{ - 3}}} \right]
C [EV2T1]\left[ {E{V^{ - 2}}{T^{ - 1}}} \right]
D [EV1T2]\left[ {E{V^{ - 1}}{T^{ - 2}}} \right]
Correct Answer
Option A
Solution

Let surface tension S =kE

aa

V b T c where k is a dimensionless constant Writing the dimensions on both sides,

[MLT2L]\left[ {{{ML{T^{ - 2}}} \over L}} \right]

=

[ML2T2]a{\left[ {M{L^2}{T^{ - 2}}} \right]^a}
[LT1]b{\left[ {L{T^{ - 1}}} \right]^b}
[T]c{\left[ T \right]^c}
[ML0T2]\left[ {M{L^0}{T^{ - 2}}} \right]

=

[MaL2a+bT2ab+c]\left[ {{M^a}{L^{2a + b}}{T^{ - 2a - b + c}}} \right]

Comparing both sides of the equation we get,

aa

= 1 ....(1) 2

aa

+ b = 0 ....(2) -2

aa

- b + c = - 2 ....(3) Solving equation (1), (2) and (3), we get

aa

= 1, b = - 2, c = - 2 \therefore Dimension of surface tension =

[EV2T2]\left[ {E{V^{ - 2}}{T^{ - 2}}} \right]
Q134
If force (F), velocity (V) and time (T) are taken as fundamental units, then dimensions of mass are
A [FVT1]\left[ {FV{T^{ - 1}}} \right]
B [FVT2]\left[ {FV{T^{ - 2}}} \right]
C [FV1T1]\left[ {F{V^{ - 1}}{T^{ - 1}}} \right]
D [FV1T]\left[ {F{V^{ - 1}}T} \right]
Correct Answer
Option D
Solution

Let mass m =kF

aa

V b T c where k is a dimensionless constant Writing the dimensions on both sides, we get

[ML0T0]\left[ {{{M{L^0}{T^{ 0}}}}} \right]

=

[MLT2]a{\left[ {M{L}{T^{ - 2}}} \right]^a}
[LT1]b{\left[ {L{T^{ - 1}}} \right]^b}
[T]c{\left[ T \right]^c}
[ML0T0]\left[ {M{L^0}{T^{0}}} \right]

=

[MaLa+bT2ab+c]\left[ {{M^a}{L^{a + b}}{T^{ - 2a - b + c}}} \right]

Comparing both sides of the equation we get,

aa

= 1 ....(1) 2

aa

+ b = 0 ....(2) -2

aa

- b + c = 0 ....(3) Solving equation (1), (2) and (3), we get

aa

= 1, b = - 1, c = 1 \therefore Dimension of mass =

[FV1T]\left[ {F{V^{ - 1}}{T}} \right]
Q135
The pair of quantities having same dimensions is
A Impulse and Surface Tension
B Angular momentum and Work
C Work and Torque
D Young's modulus and Energy
Correct Answer
Option C
Solution

Work = Force ×\times distance = [MLT -2 ][L] = [ML 2 T -2 ] Torque = Force ×\times Force arm = [MLT -2 ][L] = [ML 2 T -2 ]

Q136
If an experiment four quantities a, b, c and d are measured with percentage error 1%, 2%, 3% and 4% respectively. Quantity P is calculated as follows P =a3b2cd = {{{a^3}{b^2}} \over {cd}} % error in P is
A 7%
B 4%
C 14%
D 10%
Correct Answer
Option C
Solution

Given P

=a3b2cd= {{{a^3}{b^2}} \over {cd}}

% error in P :

ΔPP×100{{\Delta P} \over P} \times 100

=

[3Δaa+2Δbb+Δcc+Δdd]×100\left[ {3{{\Delta a} \over a} + 2{{\Delta b} \over b} + {{\Delta c} \over c} + {{\Delta d} \over d}} \right] \times 100

= 3 ×\times 1% + 2 ×\times 2% + 3% + 4% = 14%

Q137
The dimensions of (μ0ε0)1/2{\left( {{\mu _0}{\varepsilon _0}} \right)^{ - 1/2}} are
A [L1/2T1/2]\left[ {{L^{1/2}}{T^{ - 1/2}}} \right]
B [L1T]\left[ {{L^{ - 1}}T} \right]
C [LT1]\left[ {L{T^{ - 1}}} \right]
D [L1/2T1/2]\left[ {{L^{1/2}}{T^{1/2}}} \right]
Correct Answer
Option C
Solution
(μ0ε0)1/2{\left( {{\mu _0}{\varepsilon _0}} \right)^{ - 1/2}}

=

1μ0ε0{1 \over {\sqrt {{\mu _0}{\varepsilon _0}} }}

= Speed of light in vacuum = c So the dimension of

(μ0ε0)1/2{\left( {{\mu _0}{\varepsilon _0}} \right)^{ - 1/2}}

= [c] =[LT -1 ]

Q138
The damping force on an oscillator is directly proportional to the velocity. The units of the constant of proportionality are
A kg m s -1
B kg m s -2
C kg s -1
D kg s
Correct Answer
Option C
Solution

According to the question, Damping force, F \propto v \Rightarrow F = kv where k is constant of proportionality. \therefore k =

Fv{F \over v}

=

Nms1{N \over {m\,{s^{ - 1}}}}

=

kgms2ms1{{kg\,m\,{s^{ - 2}}} \over {m\,{s^{ - 1}}}}

=

kgs1kg\,{s^{ - 1}}
Q139
The density of a material in CGS system of units is 4 g cm -3 . In a system of units in which unit of length is 10 cm and unit of mass is 100 g, the value of density of material will be
A 0.04
B 0.4
C 40
D 400
Correct Answer
Option C
Solution

In CGS system, Density = 4

gcm3{g \over {c{m^3}}}

When unit of mass is 100g and unit of length is 10 cm, then Density = x

100g(10cm)3{{100g} \over {{{\left( {10cm} \right)}^3}}}

\therefore 4

gcm3{g \over {c{m^3}}}

= x

100g(10cm)3{{100g} \over {{{\left( {10cm} \right)}^3}}}

\Rightarrow x = 40 unit

Q140
The dimensions of (μ0ε0)1/2{\left( {{\mu _0}{\varepsilon _0}} \right)^{ - 1/2}} are
A [L1/2T1/2]\left[ {{L^{1/2}}{T^{ - 1/2}}} \right]
B [L1T]\left[ {{L^{ - 1}}T} \right]
C [LT1]\left[ {L{T^{ - 1}}} \right]
D [L1/2T1/2]\left[ {{L^{1/2}}{T^{1/2}}} \right]
Correct Answer
Option C
Solution
(μ0ε0)1/2{\left( {{\mu _0}{\varepsilon _0}} \right)^{ - 1/2}}

=

1μ0ε0{1 \over {\sqrt {{\mu _0}{\varepsilon _0}} }}

= Speed of light in vacuum = c So the dimension of

(μ0ε0)1/2{\left( {{\mu _0}{\varepsilon _0}} \right)^{ - 1/2}}

= [c] =[LT -1 ]

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