JEE PYQ: Units & Measurements - Question ID 4f3c5aa1ceb4 (JEE Main 2026)

ID: 4f3c5aa1ceb4JEE Main 2026Single Correct MCQ

 Match List - I with List - II. \text { Match List - I with List - II. }

<br> List - I <br><br>\text { List - I }<br>
<br> List - II <br><br>\text { List - II }<br>
A. Boltzmann constant I. <br>[M1 L3 T2]<br><br>\left[\mathrm{M}^{-1} \mathrm{~L}^3 \mathrm{~T}^{-2}\right]<br>
B. Stefan's constant II. <br>[M L2 T1]<br><br>\left[\mathrm{M} \mathrm{~L}^2 \mathrm{~T}^{-1}\right]<br>
C. Planck's constant III. <br>[ML2 T2 K1]<br><br>\left[\mathrm{ML}^2 \mathrm{~T}^{-2} \mathrm{~K}^{-1}\right]<br>
D. Gravitational constant IV. <br>[M L0 T3 K4]<br><br>\left[\mathrm{M} \mathrm{~L}^0 \mathrm{~T}^{-3} \mathrm{~K}^{-4}\right]<br>

Choose the correct answer from the options given below :

Select Option

Step-by-step Explanation

Core Formula & Concept:

In dimensional analysis, every physical constant can be expressed in terms of the fundamental dimensions: mass (M\mathrm{M}), length (L\mathrm{L}), time (T\mathrm{T}), and temperature (K\mathrm{K}). The question requires us to match four constants—Boltzmann constant (kBk_B), Stefan’s constant (σ\sigma), Planck’s constant (hh), and the gravitational constant (GG)—with their correct dimensional formulae.


Key relations used:

  • Boltzmann constant: kB=RNAk_B = \frac{R}{N_A} (gas constant per molecule), and from the ideal-gas law PV=nRTPV = nRT, we deduce [kB]=[R][NA]=[PV][nT][k_B] = \frac{[R]}{[N_A]} = \frac{[PV]}{[nT]}
  • Stefan’s law: P=σAT4P = \sigma A T^4, so [σ]=[P][A][T4][\sigma] = \frac{[P]}{[A][T^4]}
  • Planck’s constant: E=hνE = h\nu, so [h]=[E][ν][h] = \frac{[E]}{[\nu]}
  • Newton’s law of gravitation: F=Gm1m2r2F = G\frac{m_1m_2}{r^2}, so [G]=[F][r2][m1][m2][G] = \frac{[F][r^2]}{[m_1][m_2]}
Step-by-Step Derivation:

1. Boltzmann constant (kBk_B)

From the ideal-gas law PV=nRTPV = nRT, we have R=PVnT.R = \frac{PV}{nT}. Since n=NNAn = \frac{N}{N_A}, R=PVNANT=kBNA.R = \frac{PV\,N_A}{N\,T} = k_B N_A. Thus kB=RNA.k_B = \frac{R}{N_A}. Dimensionally, [R]=[P][V][T]=(ML1T2)(L3)K=ML2T2K1.[R] = \frac{[P][V]}{[T]} = \frac{(\mathrm{M\,L^{-1}\,T^{-2}})(\mathrm{L^3})}{\mathrm{K}} = \mathrm{M\,L^2\,T^{-2}\,K^{-1}}. Because NAN_A is dimensionless (count of molecules), [kB]=[R]=ML2T2K1.[k_B] = [R] = \mathrm{M\,L^2\,T^{-2}\,K^{-1}}. This matches List-II entry III.

2. Stefan’s constant (σ\sigma)

Stefan’s law states P=σAT4P = \sigma A T^4, so σ=PAT4.\sigma = \frac{P}{A\,T^4}. Dimensionally, [P]=ML2T3,[A]=L2,[T4]=K4.[P] = \mathrm{M\,L^2\,T^{-3}},\quad [A] = \mathrm{L^2},\quad [T^4] = \mathrm{K^4}. Hence [σ]=ML2T3L2K4=ML0T3K4.[\sigma] = \frac{\mathrm{M\,L^2\,T^{-3}}}{\mathrm{L^2\,K^4}} = \mathrm{M\,L^0\,T^{-3}\,K^{-4}}. This matches List-II entry IV.

3. Planck’s constant (hh)

From E=hνE = h\nu, we get h=Eν.h = \frac{E}{\nu}. Dimensionally, [E]=ML2T2,[ν]=T1.[E] = \mathrm{M\,L^2\,T^{-2}},\quad [\nu] = \mathrm{T^{-1}}. Therefore [h]=ML2T2T1=ML2T1.[h] = \frac{\mathrm{M\,L^2\,T^{-2}}}{\mathrm{T^{-1}}} = \mathrm{M\,L^2\,T^{-1}}. This matches List-II entry II.

4. Gravitational constant (GG)

Newton’s law F=Gm1m2r2F = G\frac{m_1m_2}{r^2} gives G=Fr2m1m2.G = \frac{F\,r^2}{m_1m_2}. Dimensionally, [F]=MLT2,[r2]=L2,[m1m2]=M2.[F] = \mathrm{M\,L\,T^{-2}},\quad [r^2] = \mathrm{L^2},\quad [m_1m_2] = \mathrm{M^2}. Thus [G]=MLT2L2M2=M1L3T2.[G] = \frac{\mathrm{M\,L\,T^{-2}}\cdot\mathrm{L^2}}{\mathrm{M^2}} = \mathrm{M^{-1}\,L^3\,T^{-2}}. This matches List-II entry I.

Matching the constants to their dimensions yields:

  • A (Boltzmann constant) → III
  • B (Stefan’s constant) → IV
  • C (Planck’s constant) → II
  • D (Gravitational constant) → I

This corresponds to option C.

Common Traps & Exam Tip:

Students often confuse the dimensions of Boltzmann’s constant with those of the gas constant or misapply the temperature exponent in Stefan’s law. A frequent error is swapping the dimensions of kBk_B and σ\sigma. Always derive each constant from its defining equation rather than memorising the dimensions.

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