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Question: Let \(\left[ {{\varepsilon _0}} \right]\) denotes the dimensional formula of the permittivity of vac...

Let [ε0]\left[ {{\varepsilon _0}} \right] denotes the dimensional formula of the permittivity of vacuum. If MM= mass, LL = length, TT = time and AA = electric current, then
A. [ε0]=[M1L3T4A2]\left[ {{\varepsilon _0}} \right] = \left[ {{M^{ - 1}}{L^{ - 3}}{T^4}{A^2}} \right]
B. [ε0]=[M1L2T1A2]\left[ {{\varepsilon _0}} \right] = \left[ {{M^{ - 1}}{L^2}{T^{ - 1}}{A^{ - 2}}} \right]
C. [ε0]=[M1L2T1A]\left[ {{\varepsilon _0}} \right] = \left[ {{M^{ - 1}}{L^2}{T^{ - 1}}A} \right]
D. [ε0]=[M1L3T2A]\left[ {{\varepsilon _0}} \right] = \left[ {{M^{ - 1}}{L^{ - 3}}{T^2}A} \right]

Explanation

Solution

Hint: The permittivity of vacuum [ε0]\left[ {{\varepsilon _0}} \right] and the mass, the length, time and electric current are related by Coulomb's law. By applying the force equation given in Coulomb’s law, the relation between the given parameters will be defined.
And substitute the SI unit of the term used in the relation of force by Coulomb’s law. The rearrange the equation in the form which gives the value of the permittivity of vacuum. Thus, the dimensional formula for the permittivity of vacuum can be derived.

Useful formula:
The coulomb’s law is given by,
F=14πε0×q1q2r2F = \dfrac{1}{{4\pi {\varepsilon _0}}} \times \dfrac{{{q_1}{q_2}}}{{{r^2}}}
Where, FF is the force of attraction or repulsion between the charges, ε0{\varepsilon _0} is the permittivity of vacuum or free space,q1{q_1} is the magnitude of first charge, q2{q_2} is the magnitude of second charge and rr is the separation distance between the charges q1{q_1} and q2{q_2}.

Newton’s second law of motion,
F=maF = ma
Where, FF is the force on the body, mm is the mass of the body and aa is the acceleration of the body.

The current flows through the conductor,
I=qtI = \dfrac{q}{t}
Where, II is the current flowing through the conductor, qq is the charge flowing in the conductor and tt is the time taken.

Given data:
MM= mass
LL = length
TT = time
AA = electric current

Step by step solution:
By Coulomb’s law,
F=14πε0×q1q2r2F = \dfrac{1}{{4\pi {\varepsilon _0}}} \times \dfrac{{{q_1}{q_2}}}{{{r^2}}}
Rearranging the above equation, we get
ε0=14πF×q1q2r2  .............................................(1){\varepsilon _0} = \dfrac{1}{{4\pi F}} \times \dfrac{{{q_1}{q_2}}}{{{r^2}}}\;.............................................\left( 1 \right)

By Newton’s second law of motion,
F=ma  ...................................(2)F = ma\;...................................\left( 2 \right)

The current flows through the conductor,
I=qtI = \dfrac{q}{t}
Rearranging the above equation, we get
q=It  ..........................................(3)q = It\;..........................................\left( 3 \right)
Substitute the equations (2) and (3) in equation (1), we get
ε0=14πma×I1t1×I2t2r2  ....................................(4){\varepsilon _0} = \dfrac{1}{{4\pi ma}} \times \dfrac{{{I_1}{t_1} \times {I_2}{t_2}}}{{{r^2}}}\;....................................\left( 4 \right)
Substitute the SI units on RHS of above equation (4), we get
ε0=1kg×ms2×As×Asm2  {\varepsilon _0} = \dfrac{1}{{kg \times m{s^{ - 2}}}} \times \dfrac{{As \times As}}{{{m^2}}}\;
Since, kgkg is unit of mass denoted by MM, mm is unit of length denoted by LL and ss is unit of time denoted by TT
Thus,
ε0=1M×LT2×AT×ATL2   ε0=A2T2ML3T2 ε0=M1L3T4A2  {\varepsilon _0} = \dfrac{1}{{M \times L{T^{ - 2}}}} \times \dfrac{{AT \times AT}}{{{L^2}}}\; \\\ {\varepsilon _0} = \dfrac{{{A^2}{T^2}}}{{M{L^3}{T^{ - 2}}}} \\\ {\varepsilon _0} = {M^{ - 1}}{L^{ - 3}}{T^4}{A^2} \\\

Hence, the option (A) is correct.

Note: The conventional unit of the permittivity of free space or vacuum is derived from Coulomb's law. While applying the conventional units, care should be taken more. The convention unit of mass is MM, length is LL, time is TT and current is AA. Hence, don’t get confused with the SI units and the conventional units. Both are completely different from one another.