Units & Measurements

JEE Physics · 184 questions · Page 10 of 19 · Click an option or "Show Solution" to reveal answer

Q91
If velocity [V], time [T] and force [F] are chosen as the base quantities, the dimensions of the mass will be :
A [FT-1 V-1]
B [FTV-1]
C [FT2 V]
D [FVT-1]
Correct Answer
Option B
Solution

[M] = K[F]a [T]b [V]c [M1] = [M1L1T-2]a [T1]b [L1T-1]c a = 1, b = 1, c = -1 \therefore [M] = [FTV-1]

Q92
Velocity (v) and acceleration (a) in two systems of units 1 and 2 are related as v2=nm2v1{v_2} = {n \over {{m^2}}}{v_1} and a2=a1mn{a_2} = {{{a_1}} \over {mn}} respectively. Here m and n are constants. The relations for distance and time in two systems respectively are :
A n3m3L1=L2{{{n^3}} \over {{m^3}}}{L_1} = {L_2} and n2mT1=T2{{{n^2}} \over m}{T_1} = {T_2}
B L1=n4m2L2{L_1} = {{{n^4}} \over {{m^2}}}{L_2} and T1=n2mT2{T_1} = {{{n^2}} \over m}{T_2}
C L1=n2mL2{L_1} = {{{n^2}} \over m}{L_2} and T1=n4m2T2{T_1} = {{{n^4}} \over {{m^2}}}{T_2}
D n2mL1=L2{{{n^2}} \over m}{L_1} = {L_2} and n4m2T1=T2{{{n^4}} \over {{m^2}}}{T_1} = {T_2}
Correct Answer
Option A
Solution
[L]=[v2][a][L] = {{[{v^2}]} \over {[a]}}

so

[v2]2[a2]=[nm2v1]2[a1mn]{{{{[{v_2}]}^2}} \over {[{a_2}]}} = {{{{\left[ {{n \over {{m^2}}}{v_1}} \right]}^2}} \over {\left[ {{{{a_1}} \over {mn}}} \right]}}
[v2]2[a2]=n3m3[v1]2[a1]{{{{[{v_2}]}^2}} \over {[{a_2}]}} = {{{n^3}} \over {{m^3}}}{{{{[{v_1}]}^2}} \over {[{a_1}]}}

or

[L2]=n3m3[L1][{L_2}] = {{{n^3}} \over {{m^3}}}[{L_1}]

Similarly,

[T]=[v][a][T] = {{[v]} \over {[a]}}

So,

[T2]=n2m[T1][{T_2}] = {{{n^2}} \over m}[{T_1}]
Q93
The SI unit of a physical quantity is pascal-second. The dimensional formula of this quantity will be :
A [ML-1T-1]
B [ML-1T-2]
C [ML2T-1]
D [M-1L3T0]
Correct Answer
Option A
Solution

[pascal-second] =

MLT2L2×T{{ML{T^{ - 2}}} \over {{L^2}}} \times T
=ML1T1= M{L^{ - 1}}{T^{ - 1}}
Q94
An expression for a dimensionless quantity P is given by P=αβloge(ktβx)P = {\alpha \over \beta }{\log _e}\left( {{{kt} \over {\beta x}}} \right); where α\alpha and β\beta are constants, x is distance; k is Boltzmann constant and t is the temperature. Then the dimensions of α\alpha will be :
A [M0 L-1 T0]
B [M L0 T-2]
C [M L T-2]
D [M L2 T-2]
Correct Answer
Option C
Solution

Given, P=αβloge[ktβx]P=\dfrac{\alpha}{\beta} \log _{e}\left[\dfrac{k t}{\beta x}\right] The logarithmic term is dimensionless.

Thus, [kt/βx][k t / \beta x] is also dimensionless. i.e.

[k][t][β][x]=[M0 L0 T0]\dfrac{[k][t]}{[\beta][x]}=\left[\mathrm{M}^{0} \mathrm{~L}^{0} \mathrm{~T}^{0}\right] .......(i) We have, E=ktE=k t Thus, Eq. (i) becomes,

[M1 L2 T2][β][L1]=[M0 L0 T0][β]=[MLT2]\begin{array}{r} \frac{\left[\mathrm{M}^{1} \mathrm{~L}^{2} \mathrm{~T}^{-2}\right]}{[\mathrm{\beta}]\left[\mathrm{L}^{1}\right]}=\left[\mathrm{M}^{0} \mathrm{~L}^{0} \mathrm{~T}^{0}\right] \\\\ {[\beta]=\left[\mathrm{MLT}^{-2}\right]} \end{array}

Since, PP is also a dimensionless quantity.

[α][β]=[M0 L0 T0][α]=[β][M0 L0 T0][α]=[M1 L1 T2]=[MLT2]\begin{aligned} &\frac{[\alpha]}{[\beta]}=\left[\mathrm{M}^{0} \mathrm{~L}^{0} \mathrm{~T}^{0}\right] \\\\ &{[\alpha]=[\beta]\left[\mathrm{M}^{0} \mathrm{~L}^{0} \mathrm{~T}^{0}\right]} \\\\ &{[\alpha]=\left[\mathrm{M}^{1} \mathrm{~L}^{1} \mathrm{~T}^{-2}\right]=\left[\mathrm{MLT}^{-2}\right]} \end{aligned}
Q95
The expression given below shows the variation of velocity (v) with time (t), v=At2+BtC+tv=\mathrm{At}^2+\dfrac{\mathrm{Bt}}{\mathrm{C}+\mathrm{t}}. The dimension of ABC is :
A [M0L1T−2]
B [M0L2T−3]
C [M0L2T−2]
D [M0L1T−3]
Correct Answer
Option B
Solution
[LT1]=[A][T2]=[B][T][C]+[T][C]=[T][A]=[LT3][B]=[LT1][ABC]=[L2 T3]\begin{aligned} & {\left[\mathrm{LT}^{-1}\right]=[\mathrm{A}]\left[\mathrm{T}^2\right]=\frac{[\mathrm{B}][\mathrm{T}]}{[\mathrm{C}]+[\mathrm{T}]}} \\ & {[\mathrm{C}]=[\mathrm{T}]} \\ & {[\mathrm{A}]=\left[\mathrm{LT}^{-3}\right]} \\ & {[\mathrm{B}]=\left[\mathrm{LT}^{-1}\right]} \\ & {[\mathrm{ABC}]=\left[\mathrm{L}^2 \mathrm{~T}^{-3}\right]} \end{aligned}
Q96
If n main scale divisions coincide with (n + 1) vernier scale divisions. The least count of vernier callipers, when each centimetre on the main scale is divided into five equal parts, will be :
A 2n+1{2 \over {n + 1}} mm
B 5n+1{5 \over {n + 1}} mm
C 12n{1 \over {2n}} mm
D 15n{1 \over {5n}} mm
Correct Answer
Option A
Solution

5 parts of main scale division = 1 cm \therefore 1 part of main scale division =

15{1 \over 5}

cm \therefore 1 M.S.D. =

15{1 \over 5}

cm (n + 1) vernier scale division = n main scale division. \therefore 1 V.S.D. =

nn+1{n \over n+1}

M.S.D. =

nn+1{n \over n+1}

×\times 1 M.S.D. =

nn+1{n \over n + 1}

×\times

15{1 \over 5}

cm We know, L.C. = 1 M.S.D. - 1 V,S.D. =

15{1 \over 5}

cm -

n5(n+1){n \over {5(n + 1)}}

cm =

n+1n5(n+1){{n + 1 - n} \over {5(n + 1)}}

cm =

15(n+1){1 \over {5(n + 1)}}

cm

Q97
If momentum [P], area [A][\mathrm{A}] and time [T][\mathrm{T}] are taken as fundamental quantities, then the dimensional formula for coefficient of viscosity is :
A [PA1 T0]\left[\mathrm{P} \,\mathrm{A}^{-1} \mathrm{~T}^{0}\right]
B [PA T1]\left[\mathrm{P} \,\mathrm{A}\mathrm{~T}^{-1}\right]
C [PA1 T]\left[\mathrm{P}\,\mathrm{A}^{-1} \mathrm{~T}\right]
D [PA1 T1]\left[\mathrm{P} \,\mathrm{A}^{-1} \mathrm{~T}^{-1}\right]
Correct Answer
Option A
Solution
[η]=[ML1T1][\eta ] = [M{L^{ - 1}}{T^{ - 1}}]

Now if

[η]=[P]a[A]b[T]c[\eta ] = {[P]^a}{[A]^b}{[T]^c}
[ML1T1]=[ML1T1]a[L2]b[T]c\Rightarrow [M{L^{ - 1}}{T^{ - 1}}] = {[M{L^1}{T^{ - 1}}]^a}{[{L^2}]^b}{[T]^c}
a=1,a+2b=1,a+c=1\Rightarrow a = 1,\,a + 2b = - 1,\, - a + c = - 1
a=1,b=1,c=0\Rightarrow a = 1,\,b = - 1,\,c = 0
[η]=[P][A]1[T]0\Rightarrow [\eta ] = [P]{[A]^{ - 1}}{[T]^0}
=[PA1T0]= [P{A^{ - 1}}{T^0}]
Q98
The maximum error in the measurement of resistance, current and time for which current flows in an electrical circuit are 1%,2%1 \%, 2 \% and 3%3 \% respectively. The maximum percentage error in the detection of the dissipated heat will be :
A 2
B 4
C 6
D 8
Correct Answer
Option D
Solution

Given, ΔRR×100=1%\dfrac{\Delta R}{R} \times 100=1 \%

ΔFF×100=2% and Δtt×100=3%\frac{\Delta F}{F} \times 100=2 \% \text{ and } \frac{\Delta t}{t} \times 100=3 \%

We know that, heat produced due to current flowing through a resistor RR.

H=I2Rt H =I^{2} R t ΔHH=2ΔII+ΔRR+Δtt \Rightarrow \dfrac{\Delta H}{H} =\dfrac{2 \Delta I}{I}+\dfrac{\Delta R}{R}+\dfrac{\Delta t}{t} ΔHH×100=2(ΔII×100)+ΔRR×100+Δtt×100 \Rightarrow \dfrac{\Delta H}{H} \times 100 =2\left(\dfrac{\Delta I}{I} \times 100\right)+\dfrac{\Delta R}{R} \times 100+\dfrac{\Delta t}{t} \times 100 =2×2%+1%+3%=8% =2 \times 2 \%+1 \%+3 \%=8 \%

Q99
A screw gauge of pitch 0.5 mm0.5 \mathrm{~mm} is used to measure the diameter of uniform wire of length 6.8 cm6.8 \mathrm{~cm}, the main scale reading is 1.5 mm1.5 \mathrm{~mm} and circular scale reading is 7 . The calculated curved surface area of wire to appropriate significant figures is : [Screw gauge has 50 divisions on its circular scale]
A 6.8 cm2
B 3.4 cm2
C 3.9 cm2
D 2.4 cm2
Correct Answer
Option B
Solution

Least count

=0.550= {{0.5} \over {50}}

mm = 0.01 mm \therefore Diameter, d = 1.5 mm + 7 ×\times 0.01 = 1.57 mm \therefore Surface area

=(2πr)×l= (2\pi r) \times l
=πdl= \pi dl
=3.142×1.5710×6.8= 3.142 \times {{1.57} \over {10}} \times 6.8

cm2 = 3.354 cm2 = 3.4 cm2

Q100
In a Vernier Calipers, 10 divisions of Vernier scale is equal to the 9 divisions of main scale. When both jaws of Vernier calipers touch each other, the zero of the Vernier scale is shifted to the left of zero of the main scale and 4th 4^{\text{th }} Vernier scale division exactly coincides with the main scale reading. One main scale division is equal to 1 mm1 \mathrm{~mm}. While measuring diameter of a spherical body, the body is held between two jaws. It is now observed that zero of the Vernier scale lies between 30 and 31 divisions of main scale reading and 6th 6^{\text{th }} Vernier scale division exactly coincides with the main scale reading. The diameter of the spherical body will be :
A 3.02 cm
B 3.06 cm
C 3.10 cm
D 3.20 cm
Correct Answer
Option C
Solution

Given, In Vernier calipers, 10 VSD =9=9 MSD 1\Rightarrow \quad 1 VSD =910=\dfrac{9}{10} MSD \therefore Least count of vernier scale,

 LC =1MSD1VSD=1MSD910MSD=MSD(1910)= MSD 10=1 mm10[1MSD=1 mm]=0.1 mm=0.01 cm\begin{aligned} \text{ LC } &=1 \mathrm{MSD}-1 \mathrm{VSD} \\\\ &=1 \mathrm{MSD}-\frac{9}{10} \mathrm{MSD}=\operatorname{MSD}\left(1-\frac{9}{10}\right) \\\\ &=\frac{\text{ MSD }}{10}=\frac{1 \mathrm{~mm}}{10} \quad[\because 1 \mathrm{MSD}=1 \mathrm{~mm}] \\\\ &=0.1 \mathrm{~mm}=0.01 \mathrm{~cm} \end{aligned}

According to given situation, Negative error == Main scale reading - Least count ×\times Number of coinciding main scale division

=0.10.01×4=0.10.04=0.06 cm=0.1-0.01 \times 4=0.1-0.04=0.06 \mathrm{~cm}

\therefore Diameter of spherical body

=30×0.1+6×0.01+0.06=3.0+0.06+0.06=3.12 cm\begin{aligned} &=30 \times 0.1+6 \times 0.01+0.06 \\\\ &=3.0+0.06+0.06=3.12 \mathrm{~cm} \end{aligned}

Which is closest to 3.10 cm3.10 \mathrm{~cm}.

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