NEET 2027 · Physics · Class 11 · Ch. 1 Units and Measurement
The two things you can do with a dimensional formula once you have it: test an equation for consistency, and build the form of a new relation from scratch. Plus the four things you cannot do.
Once you can write a dimensional formula, you can do two useful things with it: check whether an equation could be right, and work out the shape of a relation you have never seen.
Both rest on one idea, the principle of homogeneity: quantities can only be added or subtracted if they have the same dimensions. You can add a velocity to a velocity. You cannot add a velocity to a force, or a current to a temperature. It follows that every term in a valid physical equation must carry the identical dimensional formula.
Reduce every term of a proposed equation. If any term disagrees, the equation is wrong — certainly, finally, with no appeal. If all terms agree, the equation has passed a test but has not been proved. NCERT states the asymmetry precisely: if an equation fails this consistency test, it is proved wrong, but if it passes, it is not proved right.
The reason is that dimensions are blind to pure numbers. T = 2π√(l/g) and T = 5√(l/g) are equally consistent, and only one describes a real pendulum.
Suppose you believe a quantity depends on three others but you do not know how. Assume a product of powers, write the dimensional equation, and match the exponents of M, L and T one base quantity at a time. Three equations, three unknowns, and the form of the relation drops out.
This is the method NCERT uses to obtain T = k√(l/g) for the pendulum. It delivers the shape of the answer and never the constant.
Rule of addition: anything added or subtracted must match. Whenever you see a sum containing an unknown constant, that constant's dimensions are already determined.
Rule of special functions: whatever sits inside sin, cos, tan, log or ex is dimensionless, and so is what comes out. Angles, ratios and exponents are always pure numbers.
For x = x₀ + v₀t + ½at², all four terms reduce to L: x is L, x₀ is L, v₀t is (L T⁻¹)(T) = L, and ½at² is (L T⁻²)(T²) = L. The equation is dimensionally correct.
A dimensional check takes about fifteen seconds and catches a whole class of algebra errors — a dropped square, an inverted fraction, a term multiplied where it should have been divided. It is worth running on any formula you have manipulated yourself in a long question.
It also has an advantage over checking units: you need not commit to a particular system, and you need not worry about multiples and sub-multiples.
In most problems only one or two of the variables carry mass, so the M equation is the simplest and often fixes an exponent outright. In the pendulum problem it gives z = 0 in a single line — which is the physically interesting result that the period does not depend on the mass of the bob at all.
| Relation | Assumed dependence | Dimensional result | Constant, from elsewhere |
|---|---|---|---|
| Simple pendulum | T on l, g, m | T ∝ √(l/g) | k = 2π |
| Stokes' law | F on η, r, v | F ∝ ηrv | k = 6π |
| Speed of sound | v on E, ρ | v ∝ √(E/ρ) | k = 1 |
| Wave on a string | v on F, μ | v ∝ √(F/μ) | k = 1 |
| Oscillating liquid drop | T on ρ, r, S | T ∝ √(ρr³/S) | k found experimentally |
| Photon energy | E on h, ν | E ∝ hν | k = 1 |
| Planck length | from G, h, c | √(Gh/c³) | ≈ 1.6 × 10⁻³⁵ m |
| Limitation | Standard illustration |
|---|---|
| 1. Cannot find dimensionless constants. A pure number leaves no trace in a dimensional equation. | T = k√(l/g) is as far as the method goes; k = 2π must come from experiment. Similarly the 6π in Stokes' law. |
| 2. Cannot distinguish quantities with the same dimensions. The formula records exponents, not physical meaning or vector nature. | Work and torque are both M L² T⁻², yet one is a scalar energy transfer and the other a vector turning effect. |
| 3. Fails for sums, and for trigonometric, logarithmic or exponential relations. The method assumes a single product of powers. | s = ut + ½at² can be checked but never derived. Nor can y = A sin(ωt − kx). |
| 4. Limited to three unknowns. In mechanics only M, L and T supply equations, so at most three exponents can be found. | A quantity depending on four others cannot be pinned down without extra physical input. |
Its one-directional power is real. A dimensionally inconsistent equation is wrong, and no amount of adjusting numerical factors can save it. That makes the check a genuinely reliable filter, and it costs almost nothing to run.
NCERT adds a second advantage: a dimensional test tells you no more and no less than a test of units, but it spares you from committing to any particular system of units and from worrying about multiples and sub-multiples.
The most-tested idea in this section, usually as an assertion–reason item where both statements are true and the question is whether the reason explains the assertion.
K = ½mv² + ma can be eliminated at a glance, because energy and force have been added. Scan every option for a sum of unlike terms before computing anything.
In the relativistic mass question, m and m₀ are both masses, so the prefactor must be exactly 1. That eliminates one option before you touch the bracket.
Deriving T ∝ √(l/g) is not the same as deriving T = 2π√(l/g). If an option includes a numerical constant, ask whether dimensional analysis could possibly have supplied it.
After solving for exponents, ask whether the physics agrees. A larger surface tension should make a drop oscillate faster, so S must sit in the denominator of the period. This catches inverted answers, which are the commonest distractor.
G, h, k, σ and R all carry dimensions. Only things like 2π, ½ and counted integers are dimensionless. Treating G as a pure number breaks every gravitational check.
| Relation | Form from dimensional analysis | Constant |
|---|---|---|
| Simple pendulum | T = k√(l/g) | k = 2π |
| Stokes' law | F = kηrv | k = 6π |
| Terminal velocity | v = k r²(ρ−σ)g/η | k = 2/9 |
| Speed of sound in a solid | v = √(Y/ρ) | — |
| Speed of sound in a gas | v = √(γP/ρ) | — |
| Transverse wave on a string | v = √(F/μ) | — |
| Frequency of a stretched string | n = (1/2l)√(F/μ) | — |
| Oscillating liquid drop | T ∝ √(ρr³/S) | found experimentally |
| Escape velocity | v = √(2GM/R) | the 2 from energy conservation |
| Photon energy | E = hν | k = 1 |
| Planck length | √(Gh/c³) ≈ 1.6 × 10⁻³⁵ m | — |
| Planck time | √(Gh/c⁵) ≈ 5.4 × 10⁻⁴⁴ s | — |
| Planck mass | √(hc/G) ≈ 2.2 × 10⁻⁸ kg | — |
| Speed of light from μ₀, ε₀ | c = 1/√(μ₀ε₀) | — |
| Name | What to attach to the name |
|---|---|
| Joseph Fourier | Stated the principle of dimensional homogeneity in his 1822 treatise on heat. The founding figure of the subject. |
| Lord Rayleigh | Turned homogeneity into a working derivation technique. The 'method of dimensions' used in NCERT Example 1.5 is Rayleigh's method. |
| Edgar Buckingham | The π-theorem (1914), which says how many independent dimensionless groups a problem has. Named in passing, not examined numerically. |
| George Gabriel Stokes | Stokes' law F = 6πηrv. Dimensional analysis gives ηrv; Stokes supplied the 6π from hydrodynamics. |
| Max Planck | Constructed the Planck length, time and mass from G, h and c alone — the purest illustration of the method's reach. |
| Albert Einstein | The relativistic mass relation of NCERT Exercise 1.13, where homogeneity alone tells you where c belongs. |
| Daniel Bernoulli | Bernoulli's equation, in which every term must be a pressure — a standard homogeneity illustration. |
Items tagged PYQ here are NCERT worked examples and chapter-end exercises, which NTA has drawn on repeatedly. Every dimensional claim on this page was checked by symbolic exponent algebra before printing.
The SI unit of energy is J = kg m² s⁻². Of the formulae for kinetic energy below, which one cannot be ruled out on the basis of dimensional arguments? (a) K = m²v³ · (b) K = ½mv² · (c) K = ma · (d) K = ½mv² + ma
| (a) | Correct. |
| (b) | M² L³ T⁻³ — wrong in all three exponents. |
| (c) | M L T⁻² is force, not energy. |
| (d) | Two different dimensions have been added, which is never permitted. |
Consider the equation ½mv² = mgh, where m is mass, v velocity, g the acceleration due to gravity and h a height. Dimensionally, this equation is:
| (a) | The ½ being dimensionless is exactly why it does not matter. |
| (b) | Both sides carry M to the first power. |
| (c) | It is not h and v that are equated but the two full expressions. |
| (d) | Correct — the NCERT worked example. |
The period T of a simple pendulum is assumed to depend on its length l, the mass m of the bob and g, as T = k lẅ gʸ mẔ. Solving the dimensional equations gives:
| (a) | y has the wrong sign; g must appear in the denominator. |
| (b) | These exponents would give T ∝ l/g, whose dimensions are T², not T. |
| (c) | Correct. |
| (d) | z must be zero — nothing in the dimensional equation allows a mass dependence. |
Which of the following equations is dimensionally incorrect?
| (a) | All three terms reduce to L²T⁻². |
| (b) | Correct — the last term should carry t², not t. |
| (c) | Both terms reduce to a velocity. |
| (d) | This is the correct form of option (b). |
The viscous force on a small sphere of radius r moving with velocity v through a fluid of viscosity η is assumed to be F = k ηa rb vc. Dimensional analysis gives:
| (a) | Correct. |
| (b) | b = 2 would make the force depend on the cross-sectional area, which is not what the exponents give. |
| (c) | a = 2 contradicts the M equation, since only η carries mass. |
| (d) | c = 2 contradicts the T equation. |
The speed of sound in a medium of bulk modulus E and density ρ is proposed as v = √(E/ρ). Dimensionally this expression is:
| (a) | That is E/ρ before the square root is taken. |
| (b) | That is the reciprocal of a speed. |
| (c) | Correct — the same structure appears in v = √(γP/ρ) for a gas and v = √(T/μ) for a string. |
| (d) | M cancels completely; no mass can survive in a speed. |
The terminal velocity of a sphere falling through a viscous fluid is written as v = 2r²(ρ − σ)g / 9η. This expression is:
| (a) | It reduces exactly to L T⁻¹. |
| (b) | σ is a density like ρ, so the subtraction is legal for any value of σ. |
| (c) | Correct. |
| (d) | Subtracting two densities is perfectly legal — they have identical dimensions. |
The escape velocity from a planet of mass M and radius R is given as v = √(2GM/R). Checking dimensionally, this expression:
| (a) | That is GM/R before the square root. |
| (b) | Correct. |
| (c) | The two masses cancel exactly. |
| (d) | G has definite dimensions, M⁻¹ L³ T⁻², and the expression works precisely because of them. |
A boy recalls the relativistic mass relation almost correctly but forgets where the constant c belongs, writing m = m₀ / (1 − v²)1/2. The correct placement is:
| (a) | v²/c gives L T⁻¹, still not dimensionless. |
| (b) | v/c² gives L⁻¹ T, not dimensionless. |
| (c) | This makes m have the dimensions of momentum per unit... in any case m and m₀ must have identical dimensions, so no stray c may multiply the numerator. |
| (d) | Correct — the standard Lorentz factor. |
The method of dimensions cannot be used to determine:
| (a) | This is a standard use of the method. |
| (b) | This is the principle of homogeneity. |
| (c) | This is the conversion application. |
| (d) | Correct. |
Which of the following statements is correct?
| (a) | Numerical factors are invisible to the test, so correctness cannot be guaranteed. |
| (b) | An incorrect equation cannot be rescued; dimensional failure is decisive. |
| (c) | Correct. |
| (d) | Work and torque share M L² T⁻²; the method cannot separate them. |
The time period of oscillation of a liquid drop depends on its density ρ, radius r and surface tension S. Dimensional analysis gives T proportional to:
| (a) | b would have to be ½, which contradicts the L equation. |
| (b) | Correct. |
| (c) | This is the reciprocal — the signs of all three exponents are inverted. |
| (d) | b = 1 does not satisfy −3a + b = 0 with a = ½. |
The frequency n of a stretched string depends on its length l, tension F and mass per unit length μ. The relation n = (1/2l)√(F/μ) is:
| (a) | Correct. |
| (b) | The division by l removes exactly one L, leaving T⁻¹, not T⁻². |
| (c) | That is √(F/μ) before the division by l. |
| (d) | Dimensional consistency is independent of the system of units — that is one of its advantages. |
In the photoelectric relation E = hν, checking dimensions confirms that h has the dimensions of:
| (a) | Energy is M L² T⁻²; h carries an extra time. |
| (b) | Power is M L² T⁻³. |
| (c) | Force × length is M L² T⁻², i.e. energy again. |
| (d) | Correct — which is why Bohr's condition mvr = nh/2π is dimensionally sound. |
Dimensional analysis cannot be used to derive which of the following relations?
| (a) | Derivable in form; only the 2π must come from elsewhere. |
| (b) | Correct. |
| (c) | Derivable in form; only the 6π must come from elsewhere. |
| (d) | Derivable in form. |
A quantity is formed as √(Gh/c³), where G is the gravitational constant, h Planck's constant and c the speed of light. Its dimensions are those of:
| (a) | The Planck time is √(Gh/c⁵), with c to the fifth power. |
| (b) | Correct. |
| (c) | The Planck mass is √(hc/G). |
| (d) | The Planck energy is the Planck mass times c². |
In the equation y = A sin(ωt − kx + φ), which of the following must be dimensionless?
| (a) | Correct. |
| (b) | A and y have the dimensions of the displacement being described. |
| (c) | ω is T⁻¹ and k is L⁻¹ — both carry dimensions. |
| (d) | A carries the dimensions of y. |
In Bernoulli's equation P + ½ρv² + ρgh = constant, the terms ½ρv² and ρgh have the dimensions of:
| (a) | Energy is M L² T⁻² — these terms are energy per unit volume. |
| (b) | Force is M L T⁻². |
| (c) | Power is M L² T⁻³. |
| (d) | Correct. |
The energy E of a photon is assumed to depend on Planck's constant h and the frequency ν as E = k haνb. Dimensional analysis gives:
| (a) | a = 2 contradicts the M equation. |
| (b) | b = 2 contradicts the T equation. |
| (c) | Correct. |
| (d) | Half-powers contradict both the M and L equations. |
Two physical quantities have the same dimensional formula M L² T⁻². Dimensional analysis can tell you:
| (a) | Correct. |
| (b) | Vector nature is not encoded in a dimensional formula at all. |
| (c) | Sharing a dimensional formula does not make two quantities the same. |
| (d) | The unit name is a convention chosen to keep the two apart; dimensions cannot supply it. |