Units & Measurements

JEE Physics · 184 questions · Page 15 of 19 · Click an option or "Show Solution" to reveal answer

Q141
In an electromagnetic system, a quantity defined as the ratio of electric dipole moment and magnetic dipole moment has dimension of [MPLQTRAS]\left[\mathrm{M}^{\mathrm{P}} \mathrm{L}^{\mathrm{Q}} \mathrm{T}^R A^{\mathrm{S}}\right]. The value of P and Q are :
A 1,0-1,0
B 0,10,-1
C 1,1-1,1
D 1,11,-1
Correct Answer
Option B
Solution

Electric dipole moment (P)=q×2(\overrightarrow{\mathrm{P}})=\mathrm{q} \times 2 \ell Magnetic dipole moment (M)=IA(\overrightarrow{\mathrm{M}})=\mathrm{IA}

[PM]=[LTA L2 A]=L1 T=M0 L1 T1 A0\left[\frac{\mathrm{P}}{\mathrm{M}}\right]=\left[\frac{\mathrm{LTA}}{\mathrm{~L}^2 \mathrm{~A}}\right]=\mathrm{L}^{-1} \mathrm{~T}=\mathrm{M}^0 \mathrm{~L}^{-1} \mathrm{~T}^1 \mathrm{~A}^0

After compering values of P&Q\mathrm{P} \& \mathrm{Q} are 0,10,-1 Correct Answer : Option 4

Q142
In finding out refractive index of glass slab the following observations were made through travelling microscope 50 vernier scale division =49 MSD;20=49 \mathrm{~MSD} ; 20 divisions on main scale in each cm\mathrm{cm} For mark on paper  MSR =8.45 cm,VC=26\text{ MSR }=8.45 \mathrm{~cm}, \mathrm{VC}=26 For mark on paper seen through slab MSR=7.12 cm,VC=41\mathrm{MSR}=7.12 \mathrm{~cm}, \mathrm{VC}=41 For powder particle on the top surface of the glass slab  MSR =4.05 cm,VC=1\text{ MSR }=4.05 \mathrm{~cm}, \mathrm{VC}=1 (MSR == Main Scale Reading, VC = Vernier Coincidence) Refractive index of the glass slab is :
A 1.52
B 1.35
C 1.24
D 1.42
Correct Answer
Option D
Solution

To find the refractive index of the glass slab, we first need to calculate the actual readings using the Main Scale Reading (MSR) and Vernier Coincidence (VC), and understand how to translate these values into a measurement of the refractive index.

We will start by calculating the Least Count (LC) of the vernier calipers.

The least count (LC) of the traveling microscope is given by the formula: LC=MSDVSD \text{LC} = \text{MSD} - \text{VSD} Where MSD is the value of one main scale division and VSD is the value of one vernier scale division in terms of the main scale.

We are told 50 vernier scale divisions equal 49 main scale divisions (MSD), so 1 VSD is 4950 \dfrac{49}{50} of an MSD.

Given that 20 divisions on the main scale represent 1 cm, each main scale division (MSD) represents: 1MSD=1cm20=0.05cm 1 \, \text{MSD} = \dfrac{1 \, \text{cm}}{20} = 0.05 \, \text{cm} Therefore, the least count (LC) of the microscope is: LC=0.05cm(4950×0.05cm)=0.05cm0.049cm=0.001cm \text{LC} = 0.05 \, \text{cm} - \left( \dfrac{49}{50} \times 0.05 \, \text{cm} \right) = 0.05 \, \text{cm} - 0.049 \, \text{cm} = 0.001 \, \text{cm} Now, using the least count to find the total reading (TR) from both supplied observations: For the mark on paper, the total reading (TR) is: TR=MSR+(VC×LC) \text{TR} = \text{MSR} + (\text{VC} \times \text{LC}) TRpaper=8.45cm+(26×0.001cm)=8.45cm+0.026cm=8.476cm \text{TR}_{\text{paper}} = 8.45 \, \text{cm} + (26 \times 0.001 \, \text{cm}) = 8.45 \, \text{cm} + 0.026 \, \text{cm} = 8.476 \, \text{cm} For the mark on the paper seen through the slab, the total reading is: TRseen through slab=7.12cm+(41×0.001cm)=7.12cm+0.041cm=7.161cm \text{TR}_{\text{seen through slab}} = 7.12 \, \text{cm} + (41 \times 0.001 \, \text{cm}) = 7.12 \, \text{cm} + 0.041 \, \text{cm} = 7.161 \, \text{cm} For the powder particle on the top surface of the glass slab: TRtop surface=4.05cm+(1×0.001cm)=4.05cm+0.001cm=4.051cm \text{TR}_{\text{top surface}} = 4.05 \, \text{cm} + (1 \times 0.001 \, \text{cm}) = 4.05 \, \text{cm} + 0.001 \, \text{cm} = 4.051 \, \text{cm} The real depth (RD) observed directly is the difference between the first and third observations (mark on paper and powder particle on top surface): RD=TRpaperTRtop surface=8.476cm4.051cm=4.425cm \text{RD} = \text{TR}_{\text{paper}} - \text{TR}_{\text{top surface}} = 8.476 \, \text{cm} - 4.051 \, \text{cm} = 4.425 \, \text{cm} The apparent depth (AD) when viewed through the slab is the difference between the second and third observations: AD=TRseen through slabTRtop surface=7.161cm4.051cm=3.11cm \text{AD} = \text{TR}_{\text{seen through slab}} - \text{TR}_{\text{top surface}} = 7.161 \, \text{cm} - 4.051 \, \text{cm} = 3.11 \, \text{cm} The refractive index (nn) of the glass slab can be found using the formula: n=Real Depth (RD)Apparent Depth (AD)=4.425cm3.11cm n = \dfrac{\text{Real Depth (RD)}}{\text{Apparent Depth (AD)}} = \dfrac{4.425 \, \text{cm}}{3.11 \, \text{cm}} Calculating this gives: n=4.4253.111.42 n = \dfrac{4.425}{3.11} \approx 1.42 Therefore, the refractive index of the glass slab is approximately 1.42, which corresponds to Option D.

Q143
To find the spring constant (k)(k) of a spring experimentally, a student commits 2%2 \% positive error in the measurement of time and 1%1 \% negative error in measurement of mass. The percentage error in determining value of kk is :
A 5%
B 3%
C 1%
D 4%
Correct Answer
Option A
Solution

To determine the spring constant

kk

of a spring experimentally, we can use the formula derived from Hooke's Law and the period of oscillation for a mass-spring system:

T=2πmkT = 2 \pi \sqrt{\frac{m}{k}}

Here,

TT

is the period of oscillation,

mm

is the mass, and

kk

is the spring constant. Rearranging the formula to solve for

kk

, we get:

k=4π2mT2k = \frac{4 \pi^2 m}{T^2}

To find the error in

kk

, we have to consider the errors in both the measurements of

TT

and

mm

. Let's denote the percentage errors as follows:

ΔT/T100%=2%\Delta T / T \cdot 100\% = 2\%

(positive error)

Δm/m100%=1%\Delta m / m \cdot 100\% = -1\%

(negative error) According to the rules of error propagation, the relative error in

kk

can be found by adding the relative errors in the measurements, each multiplied by the respective powers to which they affect

kk

. Since

TT

is squared in the denominator and

mm

is linear in the numerator, the calculation is as follows:

Δkk=2ΔTT+1Δmm\frac{\Delta k}{k} = \left| -2 \cdot \frac{\Delta T}{T} \right| + \left| 1 \cdot \frac{\Delta m}{m} \right|

Substituting the percentage errors:

Δkk=20.02+1(0.01)\frac{\Delta k}{k} = \left| -2 \cdot 0.02 \right| + \left| 1 \cdot (-0.01) \right|
Δkk=0.04+0.01\frac{\Delta k}{k} = 0.04 + 0.01
Δkk=0.05\frac{\Delta k}{k} = 0.05

Thus, the percentage error in determining the value of

kk

is:

Δkk100%=5%\frac{\Delta k}{k} \cdot 100\% = 5\%

The correct answer is Option A: 5%

Q144
While measuring diameter of wire using screw gauge the following readings were noted. Main scale reading is 1 mm1 \mathrm{~mm} and circular scale reading is equal to 42 divisions. Pitch of screw gauge is 1 mm1 \mathrm{~mm} and it has 100 divisions on circular scale. The diameter of the wire is x50 mm\dfrac{x}{50} \mathrm{~mm}. The value of xx is :
A 42
B 71
C 21
D 142
Correct Answer
Option B
Solution

To determine the diameter of the wire using a screw gauge, we employ the formula: Total reading=MSR+(CSR×LC) \text{Total reading} = \text{MSR} + (\text{CSR} \times \text{LC}) where: MSR (Main Scale Reading) is the value read directly from the main scale in mm.

CSR (Circular Scale Reading) is the number of divisions observed on the circular scale.

LC (Least Count) is the value of one division on the circular scale, calculated as PitchNumber of divisions on the circular scale\dfrac{\text{Pitch}}{\text{Number of divisions on the circular scale}}.

Given: Main Scale Reading (MSR) = 1 mm1 \mathrm{~mm} Circular Scale Reading (CSR) = 42 divisions Pitch of screw gauge = 1 mm1 \mathrm{~mm} Number of divisions on circular scale = 100 First, we find the Least Count (LC): LC=PitchNumber of divisions on the circular scale=1 mm100=0.01 mm LC = \dfrac{\text{Pitch}}{\text{Number of divisions on the circular scale}} = \dfrac{1 \mathrm{~mm}}{100} = 0.01 \mathrm{~mm} Then we calculate the total measurement of the diameter of the wire: Total reading=MSR+(CSR×LC)=1 mm+(42×0.01 mm)=1 mm+0.42 mm=1.42 mm \text{Total reading} = \text{MSR} + (\text{CSR} \times \text{LC}) = 1 \mathrm{~mm} + (42 \times 0.01 \mathrm{~mm}) = 1 \mathrm{~mm} + 0.42 \mathrm{~mm} = 1.42 \mathrm{~mm} Given that the diameter of the wire is also represented as

x50 mm\frac{x}{50} \mathrm{~mm}

, we can equate this to our found total reading: 1.42 mm=x50 mm 1.42 \mathrm{~mm} = \dfrac{x}{50} \mathrm{~mm} Solving for

xx

: 1.42=x50 1.42 = \dfrac{x}{50} x=1.42×50 x = 1.42 \times 50 x=71 x = 71 Therefore, the value of

xx

is 71, which corresponds to Option B: 71.

Q145

Match with .

List - IList - II
(A) Young’s Modulus (I) M L-1 T-1
(B) Torque (II) M L-1 T-2
(C) Coefficient of Viscosity (III) M-1 L3 T-2
(D) Gravitational Constant (IV) M L2 T-2
A (A)-(I), (B)-(III), (C)-(II), (D)-(IV)
B (A)-(IV), (B)-(II), (C)-(III), (D)-(I)
C (A)-(II), (B)-(I), (C)-(IV), (D)-(III)
D (A)-(II), (B)-(IV), (C)-(I), (D)-(III)
Correct Answer
Option D
Solution

We know, Young's modulus,

E=σεE = {\sigma \over \varepsilon }
E=FAΔLL=FA(LΔL)\Rightarrow E = {{{F \over A}} \over {{{\Delta L} \over L}}} = {F \over A}\left( {{L \over {\Delta L}}} \right)
[E]=[F][A]=[M1L1T2][L2]\Rightarrow [E] = {{[F]} \over {[A]}} = {{\left[ {{M^1}{L^1}{T^{ - 2}}} \right]} \over {\left[ {{L^2}} \right]}}

(A)

[E]=[M1L1T2]\Rightarrow [E] = [{M^1}{L^{ - 1}}{T^{ - 2}}]

(B) we know, Torque = r×Fr\times F

[τ]=[r][F][\tau ] = [r][F]
=[L][M1L1T2]= [L][{M^1}{L^1}{T^{ - 2}}]
[τ]=[M1L2T2][\tau ] = [{M^1}{L^2}{T^{ - 2}}]

(C) We know,

F=μAuyF = \mu A{u \over y}

where, F = force, μ\mu = coefficient of viscosity A = area uy\dfrac{u}{y} = rate of shear deformation

μ=FyAu\Rightarrow \mu = {{Fy} \over {Au}}
[μ]=[M1L1T2][L][L2][LT1]\Rightarrow [\mu ] = {{[{M^1}{L^1}{T^{ - 2}}][L]} \over {[{L^2}][L{T^{ - 1}}]}}
[μ]=[M1L1T1]\Rightarrow [\mu ] = [{M^1}{L^{ - 1}}{T^{ - 1}}]

(D) We know,

F=Gm1m2r2F = {{G{m_1}{m_2}} \over {{r^2}}}

(Newton's law of gravitation)

G=Fr2m1m2\Rightarrow G = {{F{r^2}} \over {{m_1}{m_2}}}
[G]=[M1L1T2][L2][M2]\Rightarrow [G] = {{[{M^1}{L^1}{T^{ - 2}}][{L^2}]} \over {[{M^2}]}}
[G]=[M1L3T2]\Rightarrow [G] = [{M^{ - 1}}{L^3}{T^{ - 2}}]

Hence, option D is correct.

Q146
Match List I with List II. .tg .tg List I List II A. Torque I. Nms1^{ - 1} B. Stress II. J kg1^{ - 1} C. Latent Heat III. Nm D. Power IV. Nm2^{ - 2} Choose the correct answer from the options given below :
A A-III, B-II, C-I, D-IV
B A-III, B-IV, C-II, D-I
C A-IV, B-I, C-III, D-II
D A-II, B-III, C-I, D-IV
Correct Answer
Option B
Solution

Torque Nm\rightarrow \mathrm{Nm} Stress N/m2\rightarrow N / \mathrm{m}^{2} Latent heat J/kg\rightarrow \mathrm{J} / \mathrm{kg} Power Nm/s\rightarrow \mathrm{N} \mathrm{m} / \mathrm{s} A-III, B-IV, C-II, D-I

Q147
If BB is magnetic field and μ0\mu_0 is permeability of free space, then the dimensions of (B/μ0)\left(B / \mu_0\right) is
A MT2 A1\mathrm{MT}^{-2} \mathrm{~A}^{-1}
B L1 A\mathrm{L}^{-1} \mathrm{~A}
C ML2 T2 A1\mathrm{ML}^2 \mathrm{~T}^{-2} \mathrm{~A}^{-1}
D LT2 A1\mathrm{LT}^{-2} \mathrm{~A}^{-1}
Correct Answer
Option B
Solution

To determine the dimensions of (Bμ0)\left(\dfrac{B}{\mu_0}\right), we start with the formula for the magnetic field BB inside a solenoid: B=μ0nI B = \mu_0 n I where n=NLn = \dfrac{N}{L} is the number of turns per unit length, II is the current, and μ0\mu_0 is the permeability of free space.

Rearranging the formula gives: Bμ0=nI=NLI \dfrac{B}{\mu_0} = nI = \dfrac{N}{L}I From the above, the dimensions of (Bμ0)\left(\dfrac{B}{\mu_0}\right) are: [Bμ0]=[L1A] \left[\dfrac{B}{\mu_0}\right] = \left[L^{-1} A\right] Thus, the dimensional formula of (Bμ0)\left(\dfrac{B}{\mu_0}\right) corresponds to L1AL^{-1} \text{A}.

Q148
Given below are two statements : Statement I: In a vernier callipers, one vernier scale division is always smaller than one main scale division. Statement II : The vernier constant is given by one main scale division multiplied by the number of vernier scale divisions. In the light of the above statements, choose the correct answer from the options given below.
A Both Statement I and Statement II are false
B Statement I is true but Statement II is false
C Both Statement I and Statement II are true
D Statement I is false but Statement II is true
Correct Answer
Option B
Solution

In general, one vernier scale division is smaller than one main scale division but in some modified cases it may be not correct.

Also least count is given by one main scale division divided by number of vernier scale division for normal vernier calliper.

Hence, option 2 is correct.

Q149
The maximum percentage error in the measurment of density of a wire is [Given, mass of wire =(0.60±0.003)g=(0.60 \pm 0.003) \mathrm{g} radius of wire =(0.50±0.01)cm=(0.50 \pm 0.01) \mathrm{cm} length of wire =(10.00±0.05)cm]=(10.00 \pm 0.05) \mathrm{cm}]
A 7
B 8
C 5
D 4
Correct Answer
Option C
Solution

To determine the maximum percentage error in the density of the wire, follow these steps: The density of the wire is given by the formula for a cylinder:

ρ=mπr2l\rho = \frac{m}{\pi r^2 l}

When calculating the maximum percentage (relative) error, you add the relative errors from each variable, taking into account the power to which each variable is raised.

Thus, for density:

Δρρ=Δmm+2Δrr+Δll\frac{\Delta \rho}{\rho} = \frac{\Delta m}{m} + 2\frac{\Delta r}{r} + \frac{\Delta l}{l}

Here:

Δmm\frac{\Delta m}{m}

is the relative error in the mass.

2Δrr2\frac{\Delta r}{r}

is due to the radius being squared.

Δll\frac{\Delta l}{l}

is the relative error in the length. Now plug in the given values: Mass:

m=0.60gm = 0.60 \, \text{g}

with an error

Δm=0.003g\Delta m = 0.003 \, \text{g}
Δmm=0.0030.60=0.005\frac{\Delta m}{m} = \frac{0.003}{0.60} = 0.005

or 0.5%. Radius:

r=0.50cmr = 0.50 \, \text{cm}

with an error

Δr=0.01cm\Delta r = 0.01 \, \text{cm}
Δrr=0.010.50=0.02\frac{\Delta r}{r} = \frac{0.01}{0.50} = 0.02

or 2%. Since the radius is squared in the formula, multiply by 2:

2Δrr=2×0.02=0.042\frac{\Delta r}{r} = 2 \times 0.02 = 0.04

or 4%. Length:

l=10.00cml = 10.00 \, \text{cm}

with an error

Δl=0.05cm\Delta l = 0.05 \, \text{cm}
Δll=0.0510.00=0.005\frac{\Delta l}{l} = \frac{0.05}{10.00} = 0.005

or 0.5%. Sum these contributions to find the overall maximum relative error:

Δρρ=0.005+0.04+0.005=0.05\frac{\Delta \rho}{\rho} = 0.005 + 0.04 + 0.005 = 0.05

Converting this relative error into a percentage gives:

0.05×100%=5%0.05 \times 100\% = 5\%

Thus, the maximum percentage error in the density of the wire is 5%, which corresponds to Option C.

Q150

Match with .

List - IList - II
(A) Angular Impulse (I) M0 L2 T-2
(B) Latent Heat (II) M L2 T-3 A-1
(C) Electrical resistivity (III) M L2 T-1
(D) Electromotive force (IV) M L3 T-3 A-2
A (A)-(II), (B)-(I), (C)-(IV), (D)-(III)
B (A)-(I), (B)-(III), (C)-(IV), (D)-(II)
C (A)-(III), (B)-(I), (C)-(IV), (D)-(II)
D (A)-(III), (B)-(I), (C)-(II), (D)-(IV)
Correct Answer
Option C
Solution

Matching the quantities from List - I with their correct dimensions from List - II is crucial to understanding their physical significance.

Here is the correct matching: (A) Angular Impulse: The dimensions of angular impulse are equivalent to those of angular momentum, represented as

ML2T1M L^2 T^{-1}

.

Hence, (A) corresponds to (III).

(B) Latent Heat: Latent heat has dimensions of energy per unit mass, which simplifies to

M0L2T2M^0 L^2 T^{-2}

.

Hence, (B) corresponds to (I).

(C) Electrical resistivity: Electrical resistivity has the dimensions of resistance multiplied by length, which can be represented as

ML3T3A2M L^3 T^{-3} A^{-2}

.

Hence, (C) corresponds to (IV).

(D) Electromotive force: Electromotive force (emf) is similar to electric potential difference and has dimensions

ML2T3A1M L^2 T^{-3} A^{-1}

. Hence, (D) corresponds to (II). Therefore, the correct answer is Option C: (A)-(III) (B)-(I) (C)-(IV) (D)-(II)

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