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JEE Mains Physics · Units and Measurements

Dimensions of Mechanical and Thermal Quantities

Every quantity's dimensions come from the equation that defines it, written in mass M, length L, time T and temperature K.

Why this matters

Thirty-five PYQs, thirty-four of them multiple choice, and four from 2026. Twenty-three are match-the-list questions that pair four quantities with four dimensional formulas; six ask which pair of quantities has, or does not have, the same dimensions; the other six ask for the dimensions of one or two named quantities, from a unit, a formula or a ratio. A table learned once answers most of them in seconds.

Concept 1 of 3: Dimensions of mechanical quantities

Start from force, F=maF = ma, which is MLT−2MLT^{-2}. Almost everything else is force combined with a length, an area or a time: energy is force × length, pressure is force ÷ area, surface tension is force ÷ length. Remember the defining equation and the dimensions follow in one line.

Definition

  • Force MLT−2MLT^{-2}; energy, work and torque ML2T−2ML^{2}T^{-2}; power ML2T−3ML^{2}T^{-3}.
  • Momentum and impulse MLT−1MLT^{-1}; angular momentum and angular impulse ML2T−1ML^{2}T^{-1}.
  • Pressure, stress, every elastic modulus and energy density ML−1T−2ML^{-1}T^{-2}.
  • Surface tension and spring constant (force per length) MT−2MT^{-2}.
  • Viscosity, from F=ηA dvdxF = \eta A\,\dfrac{dv}{dx}: ML−1T−1ML^{-1}T^{-1}; its SI unit is the pascal-second.
  • A ratio of two quantities has the ratio of their dimensions.
QuantityDefining relationDimensionsSI unit
ForceF=maF = maMLT−2MLT^{-2}newton (N)
Work, energy, torqueW=Fs, τ=rFW = Fs,\ \tau = rFML2T−2ML^{2}T^{-2}J (N m for torque)
PowerP=W/tP = W/tML2T−3ML^{2}T^{-3}watt (W)
Momentum, impulsep=mv, J=Ftp = mv,\ J = FtMLT−1MLT^{-1}kg m/s or N s
Angular momentum, angular impulseL=mvr, τtL = mvr,\ \tau tML2T−1ML^{2}T^{-1}kg m²/s
Moment of inertiaI=mr2I = mr^{2}ML2ML^{2}kg m²
Pressure, stress, Young's modulus, bulk modulusF/AF/AML−1T−2ML^{-1}T^{-2}pascal (Pa)
Pressure gradientdP/dxdP/dxML−2T−2ML^{-2}T^{-2}Pa/m
Compressibility1/bulk modulus1/\text{bulk modulus}M−1LT2M^{-1}LT^{2}Pa⁻¹
Surface tension, spring constantF/l, F/xF/l,\ F/xMT−2MT^{-2}N/m
Coefficient of viscosityF=ηA dv/dxF = \eta A\,dv/dxML−1T−1ML^{-1}T^{-1}pascal-second (Pa s)
Intensity of a wavepower ÷ areaMT−3MT^{-3}W/m²
Gravitational constant GF=Gm1m2/r2F = Gm_1m_2/r^{2}M−1L3T−2M^{-1}L^{3}T^{-2}N m²/kg²
Gravitational potentialenergy ÷ massL2T−2L^{2}T^{-2}J/kg
Angular speed, frequency, velocity gradientω=θ/t, dv/dx\omega = \theta/t,\ dv/dxT−1T^{-1}s⁻¹
Each row follows from its defining relation; force, MLT⁻², is the starting point for most of them.
Practice this conceptself-check · 4 quick reps

The same idea in a real exam question:

JEE Mains · 2026 · 28 Jan 2026 Shift 2 · Q20Moderate

Example 1 · Units and Measurements · Dimensions of Mechanical and Thermal Quantities

Match List-I with List-II.
List-IList-II
(A) Coefficient of viscosity(I) [ML−1T−2]\left\lbrack ML^{-1}T^{-2} \right\rbrack
(B) Surface tension(II) [ML2T−2]\left\lbrack ML^{2}T^{-2} \right\rbrack
(C) Pressure(III) [ML0T−2]\left\lbrack ML^{0}T^{-2} \right\rbrack
(D) Surface energy(IV) [ML−1T−1]\left\lbrack ML^{-1}T^{-1} \right\rbrack
Choose the correct answer from the options given below:

Surface energy and surface tension are not the same entry

Surface tension is force per length, MT⁻². A match list that names 'surface energy' means an energy, ML²T⁻². Read the exact words before matching.

Viscosity has one power of time, pressure has two

Viscosity is ML⁻¹T⁻¹ and pressure is ML⁻¹T⁻². The two differ only in the power of T, and match lists put them side by side to catch a slip.

Concept 2 of 3: Dimensions of thermal and modern-physics constants

A constant takes whatever dimensions make its equation balance. Boltzmann's constant turns temperature into energy (E=kBTE = k_BT), so it is energy per kelvin. Planck's constant turns frequency into energy (E=hνE = h\nu), so it is energy × time. Write the equation, isolate the constant, and read off its dimensions.

Definition

  • kB=E/Tk_B = E/T: ML2T−2K−1ML^{2}T^{-2}K^{-1}. Gas constant R=PV/(nT)R = PV/(nT): ML2T−2K−1mol−1ML^{2}T^{-2}K^{-1}\text{mol}^{-1}.
  • Specific heat c=Q/(mΔT)c = Q/(m\Delta T): L2T−2K−1L^{2}T^{-2}K^{-1}. Latent heat L=Q/mL = Q/m: L2T−2L^{2}T^{-2} (no K).
  • Thermal conductivity, from Qt=kAΔTl\dfrac{Q}{t} = kA\dfrac{\Delta T}{l}: MLT−3K−1MLT^{-3}K^{-1}.
  • Stefan's constant, from PA=σT4\dfrac{P}{A} = \sigma T^{4}: MT−3K−4MT^{-3}K^{-4}.
  • Planck's constant h=E/νh = E/\nu: ML2T−1ML^{2}T^{-1}, the same as angular momentum.
  • Stopping potential is a voltage, ML2T−3A−1ML^{2}T^{-3}A^{-1}; work function is an energy, ML2T−2ML^{2}T^{-2}.
  • Rydberg constant (it gives 1/λ1/\lambda): L−1L^{-1}. Decay constant (N=N0e−λtN = N_0e^{-\lambda t}): T−1T^{-1}.
Constant or quantityEquation it comes fromDimensions
Boltzmann constant kBk_BE=32kBTE = \tfrac{3}{2}k_BTML2T−2K−1ML^{2}T^{-2}K^{-1}
Gas constant RPV=nRTPV = nRTML2T−2K−1mol−1ML^{2}T^{-2}K^{-1}\text{mol}^{-1}
Specific heat capacityQ=mcΔTQ = mc\Delta TL2T−2K−1L^{2}T^{-2}K^{-1}
Latent heatQ=mLQ = mLL2T−2L^{2}T^{-2}
No temperature in latent heat, so it differs from specific heat.
Thermal conductivityQ/t=kA ΔT/lQ/t = kA\,\Delta T/lMLT−3K−1MLT^{-3}K^{-1}
Stefan's constant σ\sigmaP/A=σT4P/A = \sigma T^{4}MT−3K−4MT^{-3}K^{-4}
Planck's constant hE=hνE = h\nuML2T−1ML^{2}T^{-1}
Work functionhν=ϕ+Kmax⁡h\nu = \phi + K_{\max}ML2T−2ML^{2}T^{-2}
Stopping potentialeV0=Kmax⁡eV_0 = K_{\max}ML2T−3A−1ML^{2}T^{-3}A^{-1}
Rydberg constant1/λ=R(1/n12−1/n22)1/\lambda = R(1/n_1^{2} - 1/n_2^{2})L−1L^{-1}
Decay constantN=N0e−λtN = N_0e^{-\lambda t}T−1T^{-1}
Each constant has the dimensions that balance its equation.
Practice this conceptself-check · 4 quick reps

The same idea in a real exam question:

JEE Mains · 2026 · 6 Apr 2026 Shift 2 · Q2Moderate

Example 2 · Units and Measurements · Dimensions of Mechanical and Thermal Quantities

Match List-I with List-II.
List-IList-II
(A) Boltzmann constant(I) [M−1L3T−2][M^{-1}L^{3}T^{-2}]
(B) Stefan's constant(II) [ML2T−1][ML^{2}T^{-1}]
(C) Planck's constant(III) [ML2T−2K−1][ML^{2}T^{-2}K^{-1}]
(D) Gravitational constant(IV) [ML0T−3K−4][ML^{0}T^{-3}K^{-4}]
Choose the correct answer from the options given below.

Stopping potential is a voltage, not an energy

The stopping potential V₀ satisfies eV₀ = K_max, so V₀ itself is energy per charge, ML²T⁻³A⁻¹. Only eV₀ is an energy. The work function, by contrast, is an energy, ML²T⁻².

Specific heat carries K⁻¹, latent heat does not

Specific heat is energy per mass per kelvin, L²T⁻²K⁻¹. Latent heat is energy per mass, L²T⁻². They are a standard 'different dimensions' pair.

Concept 3 of 3: Pairs of quantities with the same dimensions

Different physical ideas can share dimensions. Torque and energy are both force × length; Planck's constant and angular momentum are both energy × time. To test a pair, write both dimensional formulas and compare every power. One power out of place makes the pair different.

Definition

  • Same: torque and energy; Planck's constant and angular momentum; pressure, stress, Young's modulus and energy density; velocity gradient, decay constant, angular speed and frequency; impulse and momentum.
  • Different: specific heat and latent heat; linear momentum and torque; surface tension and impulse.
  • A product such as pressure × time is viscosity: ML−1T−2×T=ML−1T−1ML^{-1}T^{-2} \times T = ML^{-1}T^{-1}.
  • uG\sqrt{uG}, with u an energy density, is ML−1T−2⋅M−1L3T−2=LT−2\sqrt{ML^{-1}T^{-2} \cdot M^{-1}L^{3}T^{-2}} = LT^{-2}: force per unit mass.
PairDimensions of the firstDimensions of the secondSame?
Torque and energyML2T−2ML^{2}T^{-2}ML2T−2ML^{2}T^{-2}Yes
Planck's constant and angular momentumML2T−1ML^{2}T^{-1}ML2T−1ML^{2}T^{-1}Yes
Stress and energy densityML−1T−2ML^{-1}T^{-2}ML−1T−2ML^{-1}T^{-2}Yes
Velocity gradient and decay constantT−1T^{-1}T−1T^{-1}Yes
Pressure × time and viscosityML−1T−1ML^{-1}T^{-1}ML−1T−1ML^{-1}T^{-1}Yes
Specific heat and latent heatL2T−2K−1L^{2}T^{-2}K^{-1}L2T−2L^{2}T^{-2}No
The only difference is K⁻¹.
Linear momentum and torqueMLT−1MLT^{-1}ML2T−2ML^{2}T^{-2}No
Surface tension and impulseMT−2MT^{-2}MLT−1MLT^{-1}No
Compare every power of M, L, T and K; one mismatch makes the pair different.
Practice this conceptself-check · 4 quick reps

The same idea in a real exam question:

JEE Mains · 2025 · 29 Jan 2025 · Q4Moderate

Example 3 · Units and Measurements · Dimensions of Mechanical and Thermal Quantities

The pair of physical quantities not having same dimensions is :

Same dimensions do not mean the same quantity

Torque and work are both ML²T⁻², but torque is not an energy: it is a turning effect, and it is not measured in joules. A statement that they 'have the same dimensions' is true; one that they 'are the same quantity' is not.

Summary — formulas & gotchas at a glance

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Reference tables (3)

Dimensions of mechanical quantities15 rows
QuantityDefining relationDimensionsSI unit
ForceF=maF = maMLT−2MLT^{-2}newton (N)
Work, energy, torqueW=Fs, τ=rFW = Fs,\ \tau = rFML2T−2ML^{2}T^{-2}J (N m for torque)
PowerP=W/tP = W/tML2T−3ML^{2}T^{-3}watt (W)
Momentum, impulsep=mv, J=Ftp = mv,\ J = FtMLT−1MLT^{-1}kg m/s or N s
Angular momentum, angular impulseL=mvr, τtL = mvr,\ \tau tML2T−1ML^{2}T^{-1}kg m²/s
Moment of inertiaI=mr2I = mr^{2}ML2ML^{2}kg m²
Pressure, stress, Young's modulus, bulk modulusF/AF/AML−1T−2ML^{-1}T^{-2}pascal (Pa)
Pressure gradientdP/dxdP/dxML−2T−2ML^{-2}T^{-2}Pa/m
Compressibility1/bulk modulus1/\text{bulk modulus}M−1LT2M^{-1}LT^{2}Pa⁻¹
Surface tension, spring constantF/l, F/xF/l,\ F/xMT−2MT^{-2}N/m
Coefficient of viscosityF=ηA dv/dxF = \eta A\,dv/dxML−1T−1ML^{-1}T^{-1}pascal-second (Pa s)
Intensity of a wavepower ÷ areaMT−3MT^{-3}W/m²
Gravitational constant GF=Gm1m2/r2F = Gm_1m_2/r^{2}M−1L3T−2M^{-1}L^{3}T^{-2}N m²/kg²
Gravitational potentialenergy ÷ massL2T−2L^{2}T^{-2}J/kg
Angular speed, frequency, velocity gradientω=θ/t, dv/dx\omega = \theta/t,\ dv/dxT−1T^{-1}s⁻¹
Each row follows from its defining relation; force, MLT⁻², is the starting point for most of them.
Dimensions of thermal and modern-physics constants11 rows
Constant or quantityEquation it comes fromDimensions
Boltzmann constant kBk_BE=32kBTE = \tfrac{3}{2}k_BTML2T−2K−1ML^{2}T^{-2}K^{-1}
Gas constant RPV=nRTPV = nRTML2T−2K−1mol−1ML^{2}T^{-2}K^{-1}\text{mol}^{-1}
Specific heat capacityQ=mcΔTQ = mc\Delta TL2T−2K−1L^{2}T^{-2}K^{-1}
Latent heatQ=mLQ = mLL2T−2L^{2}T^{-2}
No temperature in latent heat, so it differs from specific heat.
Thermal conductivityQ/t=kA ΔT/lQ/t = kA\,\Delta T/lMLT−3K−1MLT^{-3}K^{-1}
Stefan's constant σ\sigmaP/A=σT4P/A = \sigma T^{4}MT−3K−4MT^{-3}K^{-4}
Planck's constant hE=hνE = h\nuML2T−1ML^{2}T^{-1}
Work functionhν=ϕ+Kmax⁡h\nu = \phi + K_{\max}ML2T−2ML^{2}T^{-2}
Stopping potentialeV0=Kmax⁡eV_0 = K_{\max}ML2T−3A−1ML^{2}T^{-3}A^{-1}
Rydberg constant1/λ=R(1/n12−1/n22)1/\lambda = R(1/n_1^{2} - 1/n_2^{2})L−1L^{-1}
Decay constantN=N0e−λtN = N_0e^{-\lambda t}T−1T^{-1}
Each constant has the dimensions that balance its equation.
Pairs of quantities with the same dimensions8 rows
PairDimensions of the firstDimensions of the secondSame?
Torque and energyML2T−2ML^{2}T^{-2}ML2T−2ML^{2}T^{-2}Yes
Planck's constant and angular momentumML2T−1ML^{2}T^{-1}ML2T−1ML^{2}T^{-1}Yes
Stress and energy densityML−1T−2ML^{-1}T^{-2}ML−1T−2ML^{-1}T^{-2}Yes
Velocity gradient and decay constantT−1T^{-1}T−1T^{-1}Yes
Pressure × time and viscosityML−1T−1ML^{-1}T^{-1}ML−1T−1ML^{-1}T^{-1}Yes
Specific heat and latent heatL2T−2K−1L^{2}T^{-2}K^{-1}L2T−2L^{2}T^{-2}No
The only difference is K⁻¹.
Linear momentum and torqueMLT−1MLT^{-1}ML2T−2ML^{2}T^{-2}No
Surface tension and impulseMT−2MT^{-2}MLT−1MLT^{-1}No
Compare every power of M, L, T and K; one mismatch makes the pair different.

Watch out for (5)

Test yourself on Units and Measurements

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