Units & Measurements

NEET Physics · 152 questions · Page 11 of 16 · Click an option or "Show Solution" to reveal answer

Q101
Each side of a metallic cube of mass 5.580 kg is measured to the 9.0 cm . Keeping the significant figures in view, the density of the material of the cube can be best expressed as X×103 kg m3X \times 10^3 \mathrm{~kg} \mathrm{~m}^{-3} where the value of XX is:
A 7.654
B 7.6
C 7.65
D 7.7
Correct Answer
Option B
Solution

Mass of cube: m=5.580 kgm = 5.580 \text{ kg} (4 significant figures) Side of cube: a=9.0 cm=9.0×102 ma = 9.0 \text{ cm} = 9.0 \times 10^{-2} \text{ m} (2 significant figures)

V=a3=(9.0×102)3 m3V = a^3 = (9.0 \times 10^{-2})^3 \text{ m}^3
V=729×106 m3=7.29×104 m3V = 729 \times 10^{-6} \text{ m}^3 = 7.29 \times 10^{-4} \text{ m}^3
ρ=mV=5.5807.29×104 kg/m3\rho = \frac{m}{V} = \frac{5.580}{7.29 \times 10^{-4}} \text{ kg/m}^3
ρ=7654.3 kg/m3=7.6543×103 kg/m3\rho = 7654.3 \text{ kg/m}^3 = 7.6543 \times 10^3 \text{ kg/m}^3

According to NCERT rules, in multiplication or division, the final result should have the same number of significant figures as the quantity with the least number of significant figures.

Mass has 4 significant figures.

Side has only 2 significant figures.

So, the answer must be rounded off to 2 significant figures .

ρ=7.6×103 kg/m3\rho = 7.6 \times 10^3 \text{ kg/m}^3

Final Answer

X=7.6\boxed{X = 7.6}

The correct option is (B) 7.6

Q102
In a vernier calliper, 20 VSD coincide with 16 MSD (each division of length 1 mm ). The least count of the vernier callipers is:
A 0.2 cm
B 0.01 cm
C 0.02 cm
D 0.1 cm
Correct Answer
Option C
Solution

Least count of a vernier calliper The least count (L.C.) is the smallest measurement a vernier calliper can read.

It is given by:

L.C.=1MSD1VSD...(i)\text{L.C.} = 1\,\text{MSD} - 1\,\text{VSD} \quad ...(i)

It is given that 20 vernier scale divisions (VSD) coincide with 16 main scale divisions (MSD).

Each MSD is 1 mm long.

So,

20VSD=16MSD20\,\text{VSD} = 16\,\text{MSD}

Dividing both sides by 20, we get

1VSD=1620MSD1\,\text{VSD} = \frac{16}{20}\,\text{MSD}

Substitute this value in equation (i):

L.C.=1MSD1620MSD\text{L.C.} = 1\,\text{MSD} - \frac{16}{20}\,\text{MSD}

Simplifying,

L.C.=420MSD\text{L.C.} = \frac{4}{20}\,\text{MSD}

Since 1 MSD = 1 mm,

L.C.=15mm=0.2mm\text{L.C.} = \frac{1}{5}\,\text{mm} = 0.2\,\text{mm}

In centimetre, the least count is:

L.C.=0.02cm\text{L.C.} = 0.02\,\text{cm}
Q103
A balloon is made of a material of surface tension SS and its inflation outlet (from where gas is filled in it) has small area AA. It is filled with a gas of density ρ\rho and takes a spherical shape of radius RR. When the gas is allowed to flow freely out of it, its radius rr changes from RR to 0 (zero) in time TT. If the speed v(r)v(r) of gas coming out of the balloon depends on rr as rαr^\alpha and TSαAβργRδT \propto S^\alpha A^\beta \rho^\gamma R^\delta then
A a=12,α=12,β=1,γ=12,δ=72a=-\dfrac{1}{2}, \alpha=-\dfrac{1}{2}, \beta=-1, \gamma=\dfrac{1}{2}, \delta=\dfrac{7}{2}
B a=12,α=12,β=12,γ=12,δ=72a=\dfrac{1}{2}, \alpha=\dfrac{1}{2}, \beta=-\dfrac{1}{2}, \gamma=\dfrac{1}{2}, \delta=\dfrac{7}{2}
C a=12,α=12,β=1,γ=+1,δ=32a=\dfrac{1}{2}, \alpha=\dfrac{1}{2}, \beta=-1, \gamma=+1, \delta=\dfrac{3}{2}
D a=12,α=12,β=1,γ=12,δ=52a=-\dfrac{1}{2}, \alpha=-\dfrac{1}{2}, \beta=-1, \gamma=-\dfrac{1}{2}, \delta=\dfrac{5}{2}
Correct Answer
Option A
Solution

The relationship for T T is given by: TSαAβργRδ T \propto S^\alpha A^\beta \rho^\gamma R^\delta To find constants α \alpha , β \beta , γ \gamma , and δ \delta , analyze the dimensional formulae: Dimension analysis for Time T T : M0L0T1=(MT2)α(L2)β(ML3)γLδ \text{M}^0 \text{L}^0 \text{T}^1 = \left(\text{M} \text{T}^{-2}\right)^\alpha \left(\text{L}^2\right)^\beta \left(\text{M} \text{L}^{-3}\right)^\gamma \text{L}^\delta Equate dimensions: M0L0T1=Mα+γL2β3γ+δT2α \text{M}^0 \text{L}^0 \text{T}^1 = \text{M}^{\alpha + \gamma} \text{L}^{2\beta - 3\gamma + \delta} \text{T}^{-2\alpha} From comparing dimensions: For mass (M): α+γ=0\alpha + \gamma = 0 For length (L): 2β3γ+δ=02\beta - 3\gamma + \delta = 0 For time (T): 2α=1α=12 -2\alpha = 1 \Rightarrow \alpha = -\dfrac{1}{2} Solving equations: Using α=12\alpha = -\dfrac{1}{2}, α+γ=012+γ=0γ=12 \alpha + \gamma = 0 \Rightarrow -\dfrac{1}{2} + \gamma = 0 \Rightarrow \gamma = \dfrac{1}{2} Substituting these into the equation for length: 2β3(12)+δ=0 2\beta - 3\left(\dfrac{1}{2}\right) + \delta = 0 Assume β=1\beta = -1 to solve for δ\delta: 2(1)32+δ=0δ=72 2(-1) - \dfrac{3}{2} + \delta = 0 \quad \Rightarrow \quad \delta = \dfrac{7}{2} By this analysis, the values are α=12\alpha = -\dfrac{1}{2}, β=1\beta = -1, γ=12\gamma = \dfrac{1}{2}, and δ=72\delta = \dfrac{7}{2}.

Q104
A physical quantity PP is related to four observations a,b,ca, b, c and dd as follows: P=a3b2/cdP=a^3 b^2 / c \sqrt{d} The percentage errors of measurement in a,b,ca, b, c and dd are 1%,3%,2%1 \%, 3 \%, 2 \%, and 4%4 \% respectively. The percentage error in the quantity PP is
A 13%13 \%
B 15%15 \%
C 10%10 \%
D 2%2 \%
Correct Answer
Option A
Solution

The physical quantity P P is defined in terms of four observations a,b,c, a, b, c, and d d by the formula: P=a3b2cd P = \dfrac{a^3 b^2}{c \sqrt{d}} To find the percentage error in P P , we use the formula for maximum percentage error.

The general rule for percentage errors when a quantity is a product or a quotient is to add the percentage errors, while for powers, multiply the error by the power.

The percentage error for P P is calculated using: Maximum % error in P=3(Δaa×100)+2(Δbb×100)+(Δcc×100)+12(Δdd×100) \text{Maximum } \% \text{ error in } P = 3 \left( \dfrac{\Delta a}{a} \times 100 \right) + 2 \left( \dfrac{\Delta b}{b} \times 100 \right) + \left( \dfrac{\Delta c}{c} \times 100 \right) + \dfrac{1}{2} \left( \dfrac{\Delta d}{d} \times 100 \right) Given the percentage errors: a a has a percentage error of 1% 1\% b b has a percentage error of 3% 3\% c c has a percentage error of 2% 2\% d d has a percentage error of 4% 4\% Substituting these into the formula: =3×(1)+2×(3)+(2)+12×(4) = 3 \times (1) + 2 \times (3) + (2) + \dfrac{1}{2} \times (4) =3+6+2+2 = 3 + 6 + 2 + 2 =13% = 13\% Thus, the percentage error in the quantity P P is 13% 13\% .

Q105
Consider the diameter of a spherical object being measured with the help of a Vernier callipers. Suppose its 10 Vernier Scale Divisions (V.S.D.) are equal to its 9 Main Scale Divisions (M.S.D.). The least division in the M.S. is 0.1 cm and the zero of V.S. is at x=0.1 cmx=0.1 \mathrm{~cm} when the jaws of Vernier callipers are closed. If the main scale reading for the diameter is M=5 cmM=5 \mathrm{~cm} and the number of coinciding vernier division is 8 , the measured diameter after zero error correction, is
A 4.98 cm
B 5.00 cm
C 5.18 cm
D 5.08 cm
Correct Answer
Option A
Solution

To measure the diameter of a spherical object with Vernier calipers, consider the following details: Vernier Scale and Main Scale Relationship : 10 Vernier Scale Divisions (V.S.D.) are equivalent to 9 Main Scale Divisions (M.S.D.).

Least Value on Main Scale : 0.1 cm Zero Error : The zero marking on the Vernier Scale (V.S.) is at 0.1 cm when the caliper jaws are closed.

Given measurements: Main Scale Reading : M=5cm M = 5 \, \text{cm} Coinciding Vernier Division : 8 Calculations : Determining the Least Count : Least Count=1 MSD1 VSD \text{Least Count} = \text{1 MSD} - \text{1 VSD} =1×0.1cm910×0.1cm = 1 \times 0.1 \, \text{cm} - \dfrac{9}{10} \times 0.1 \, \text{cm} =0.1cm0.09cm=0.01cm = 0.1 \, \text{cm} - 0.09 \, \text{cm} = 0.01 \, \text{cm} Accounting for Zero Error : Zero Error = +0.1 cm Vernier Scale Reading Calculation : =8×0.01cm=0.08cm = 8 \times 0.01 \, \text{cm} = 0.08 \, \text{cm} Final Diameter Measurement After Zero Error Correction : Measured Diameter=Main Scale Reading+Vernier ReadingZero Error \text{Measured Diameter} = \text{Main Scale Reading} + \text{Vernier Reading} - \text{Zero Error} =5cm+0.08cm0.1cm = 5 \, \text{cm} + 0.08 \, \text{cm} - 0.1 \, \text{cm} =4.98cm = 4.98 \, \text{cm} Thus, the corrected measurement for the diameter is 4.98 cm.

Q106
In an electrical circuit, the voltage is measured as V=(200±4)V=(200 \pm 4) volt and the current is measured as I=(20±0.2)I=(20 \pm 0.2) A. The value of the resistance is:
A (10±4.2)Ω(10 \pm 4.2) \Omega
B (10±0.3)Ω(10 \pm 0.3) \Omega
C (10±0.1)Ω(10 \pm 0.1) \Omega
D (10±0.8)Ω(10 \pm 0.8) \Omega
Correct Answer
Option B
Solution

To determine the resistance

RR

using Ohm's law, we use the formula:

R=VIR = \frac{V}{I}

Given:

V=(200±4)V = (200 \pm 4)

volts

I=(20±0.2)I = (20 \pm 0.2)

amperes First, calculate the nominal value of the resistance:

R=20020=10ΩR = \frac{200}{20} = 10 \, \Omega

Next, we need to calculate the uncertainty in the resistance.

For division, the relative uncertainties add up.

The relative uncertainty for voltage is:

ΔVV=4200=0.02\frac{\Delta V}{V} = \frac{4}{200} = 0.02

and for current:

ΔII=0.220=0.01\frac{\Delta I}{I} = \frac{0.2}{20} = 0.01

Adding these relative uncertainties gives us the relative uncertainty for the resistance:

ΔRR=ΔVV+ΔII=0.02+0.01=0.03\frac{\Delta R}{R} = \frac{\Delta V}{V} + \frac{\Delta I}{I} = 0.02 + 0.01 = 0.03

Now, we calculate the absolute uncertainty for the resistance:

ΔR=R×0.03=10×0.03=0.3Ω\Delta R = R \times 0.03 = 10 \times 0.03 = 0.3 \, \Omega

Therefore, the resistance with its uncertainty is:

R=10±0.3ΩR = 10 \pm 0.3 \, \Omega

Thus, the correct answer is: Option B

(10±0.3)Ω(10 \pm 0.3) \Omega
Q107
The pitch of an error free screw gauge is 1 mm1 \mathrm{~mm} and there are 100 divisions on the circular scale. While measuring the diameter of a thick wire, the pitch scale reads 1 mm1 \mathrm{~mm} and 63rd 63^{\text{rd }} division on the circular scale coincides with the reference line. The diameter of the wire is:
A 1.63 cm1.63 \mathrm{~cm}
B 0.163 cm0.163 \mathrm{~cm}
C 0.163 m0.163 \mathrm{~m}
D 1.63 m1.63 \mathrm{~m}
Correct Answer
Option B
Solution

To determine the diameter of the wire using the screw gauge, we need to consider both the pitch scale reading and the circular scale reading.

The formula to calculate the diameter is:

D=P+(C×L)D = P + (C \times L)

Where:

DD

is the diameter of the wire.

PP

is the pitch scale reading.

CC

is the circular scale reading.

LL

is the least count of the screw gauge. Given: Pitch of the screw gauge,

P=1 mmP = 1 \mathrm{~mm}

Number of divisions on the circular scale = 100 Pitch scale reading,

P=1 mmP = 1 \mathrm{~mm}

The circular scale reads

63rd63^{\text{rd}}

division. First, we calculate the least count of the screw gauge:

L=PitchNumber of divisions=1 mm100=0.01 mmL = \frac{ \text{Pitch} }{ \text{Number of divisions} } = \frac{ 1 \mathrm{~mm} }{ 100 } = 0.01 \mathrm{~mm}

Next, we substitute the values into the formula for the diameter:

D=1 mm+(63×0.01 mm)D = 1 \mathrm{~mm} + (63 \times 0.01 \mathrm{~mm})

Calculate the product:

63×0.01 mm=0.63 mm63 \times 0.01 \mathrm{~mm} = 0.63 \mathrm{~mm}

Now, add the pitch scale reading and the circular scale reading:

D=1 mm+0.63 mm=1.63 mmD = 1 \mathrm{~mm} + 0.63 \mathrm{~mm} = 1.63 \mathrm{~mm}

Convert

1.63 mm1.63 \mathrm{~mm}

to centimeters:

1.63 mm=0.163 cm1.63 \mathrm{~mm} = 0.163 \mathrm{~cm}

Therefore, the diameter of the wire is: Option B:

0.163 cm0.163 \mathrm{~cm}
Q108
The potential energy of a particle moving along xx-direction varies as V=Ax2x+BV=\dfrac{A x^2}{\sqrt{x}+B}. The dimensions of A2B\dfrac{A^2}{B} are:
A [M3/2 L1/2 T3]\left[\mathrm{M}^{3 / 2} \mathrm{~L}^{1 / 2} \mathrm{~T}^{-3}\right]
B [M1/2LT3]\left[\mathrm{M}^{1 / 2} \mathrm{LT}^{-3}\right]
C [M2L1/2T4]\left[M^2 L^{1 / 2} T^{-4}\right]
D [ML2 T4]\left[\mathrm{ML}^2 \mathrm{~T}^{-4}\right]
Correct Answer
Option C
Solution

To determine the dimensions of

A2B\frac{A^2}{B}

, we start with the given potential energy expression:

V=Ax2x+BV = \frac{A x^2}{\sqrt{x} + B}

The dimensions of potential energy (

VV

) are

[ML2T2][ML^2T^{-2}]

.

So, we need to consider the dimensions of the other terms in the expression to match these dimensions.

Let's break it down step-by-step.

For the term

x\sqrt{x}

, where

xx

represents distance:

x\sqrt{x}

has dimensions

[L1/2][L^{1/2}]

Since both terms in the denominator

x+B\sqrt{x} + B

have to be of the same dimensions for them to be added together, the dimensions of

BB

must also be

[L1/2][L^{1/2}]

. Now the expression becomes:

V=Ax2L1/2V = \frac{A x^2}{L^{1/2}}

Thus, the dimensions must be:

[V]=[Ax2L1/2][V] = \left[\frac{A x^2}{L^{1/2}}\right]

Substitute the dimensions of

VV

,

xx

, and

LL

:

[ML2T2]=[AL2L1/2][ML^2T^{-2}] = \left[\frac{A L^2}{L^{1/2}}\right]

Simplifying the right-hand side:

[ML2T2]=[AL3/2][ML^2T^{-2}] = [A L^{3/2}]

Therefore, the dimensions of

AA

must be:

[A]=[ML2T2][L3/2][A] = [ML^2T^{-2}] \cdot [L^{-3/2}]
[A]=[ML1/2T2][A] = [ML^{1/2} T^{-2}]

We have dimensions of

AA

and

BB

. Now we need to find the dimensions of

A2B\frac{A^2}{B}

:

[A2]=[ML1/2T2]2[A^2] = [ML^{1/2} T^{-2}]^2
[A2]=[M2LT4][A^2] = [M^2 L T^{-4}]

Divide by the dimensions of

BB

:

[A2B]=[M2LT4L1/2]\left[\frac{A^2}{B}\right] = \left[\frac{M^2 L T^{-4}}{L^{1/2}}\right]
[A2B]=[M2L1/2T4]\left[\frac{A^2}{B}\right] = [M^2 L^{1/2} T^{-4}]

Thus, the dimensions of

A2B\frac{A^2}{B}

are: Option C:

[M2L1/2T4]\left[M^2 L^{1/2} T^{-4}\right]
Q109
In a vernier callipers, (N+1)(N+1) divisions of vernier scale coincide with NN divisions of main scale. If 1 MSD1 \mathrm{~MSD} represents 0.1 mm0.1 \mathrm{~mm}, the vernier constant (in cm\mathrm{cm}) is:
A 110 N\dfrac{1}{10 \mathrm{~N}}
B 1100(N+1)\dfrac{1}{100(N+1)}
C 00 N00 \mathrm{~N}
D 10(N+1)10(N+1)
Correct Answer
Option B
Solution

V.C = MSD - VSD ..... (1) given :

(N+1)VSD=N(N+1) \mathrm{VSD}=N

MSD

VSD=(NN+1)MSD\mathrm{VSD}=\left(\frac{N}{N+1}\right) \mathrm{MSD}

..... (2) From (1) and (2)

V.C=(MSD)NN+1(MSD)=MSD(1NN+1)=MSDN+1=0.01N+1=1100(N+1)\begin{aligned} & V . C=(M S D)-\frac{N}{N+1}(M S D) \\ & =M S D\left(1-\frac{N}{N+1}\right)=\frac{M S D}{N+1} \\ & =\frac{0.01}{N+1}=\frac{1}{100(N+1)} \end{aligned}
Q110
The quantities which have the same dimensions as those of solid angle are:
A strain and angle
B stress and angle
C strain and arc
D angular speed and stress
Correct Answer
Option A
Solution

Solid angle

dΩ=dAr2d \Omega=\frac{d A}{r^2}

has dimensions

[M0 L0 T0][\mathrm{M}^0 \mathrm{~L}^0 \mathrm{~T}^0]

Strain

=Δll=\frac{\Delta l}{l}

has dimensions

[M0 L0 T0][\mathrm{M}^0 \mathrm{~L}^0 \mathrm{~T}^0]

Angle measured in radians is also dimensionless

[M0 L0 T0][\mathrm{M}^0 \mathrm{~L}^0 \mathrm{~T}^0]
θ=Ir\theta=\frac{I}{r}
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