Units and Measurements
1. What This Chapter Covers
NCERT Physics Part I, Chapter 1 (Reprint 2026-27) has six sections. Note section 1.3.3 — it is where uncertainty now lives.
| Textbook section | Topic | What it answers |
|---|---|---|
| 1.1 | Introduction | Why physics needs an agreed system of units |
| 1.2 | The International System of Units | What SI is, and how its base units are fixed today |
| 1.3 | Significant figures | How many digits of a measurement you can trust |
| 1.3.3 | Uncertainty in a result | How error carries through a calculation |
| 1.4 | Dimensions of physical quantities | What a quantity's "dimensions" mean |
| 1.5 | Dimensional formulae and equations | How to write them down |
| 1.6 | Dimensional analysis | What the method can and cannot do |
What changed — and what did NOT
The old standalone "Errors in measurement" section is gone. Uncertainty is not. It survives as section 1.3.3, folded inside significant figures — and the CBSE 2026-27 syllabus lists it explicitly:
"significant figures, Determining the uncertainty in result. Dimensions of physical quantities, dimensional analysis and its applications." — CBSE Class XI Physics (Code 042), Unit I, session 2026-27
| Topic | Status in the 2026-27 chapter |
|---|---|
| Uncertainty in a calculated result | In — textbook section 1.3.3, and examinable |
Relative error, and the ± notation | In — worked in textbook section 1.3.3 |
| Combination-of-errors rule for a product | In — worked in textbook section 1.3.3 |
| Systematic / random / gross error classification | Not in this chapter |
| The terms "absolute error", "percentage error" | Not used |
| Measuring instruments as a taught section | Removed from the body |
| Vernier callipers, screw gauge | Only in Exercises 1.6 and 1.8 — never taught |
Two traps follow from this table.
- Notes that tell you error analysis is off-syllabus are wrong — CBSE lists it as examinable. Section 6 below teaches section 1.3.3 in full.
- Notes that drill you on systematic vs random errors are teaching an older edition. That classification is genuinely absent here.
Exercises 1.6 and 1.8 assume instruments the chapter never explains. Section 8 covers them.
2. Units and the SI System (Textbook 1.1 to 1.2)
Why units exist at all
A measurement is a comparison against an agreed standard. "The length is 5" means nothing until you say 5 of what.
Every quantity in physics can be built from a small independent set. So you only need units for that set.
| Term | Meaning | Examples |
|---|---|---|
| Base quantity | Independent, not built from others | length, mass, time |
| Base unit | The unit of a base quantity | metre, kilogram, second |
| Derived unit | Combination of base units | m/s, kg·m/s², N, J |
| System of units | The complete set, base + derived | SI, CGS, FPS, MKS |
Before SI
Three systems were in common use side by side:
| System | Length | Mass | Time |
|---|---|---|---|
| CGS | centimetre | gram | second |
| FPS (British) | foot | pound | second |
| MKS | metre | kilogram | second |
SI — Système International d'Unités — replaced them internationally. It was last revised in November 2018 by the General Conference on Weights and Measures.
3. The Seven Base Units, and the 2018 Redefinition (Textbook 1.2)
This is the most quietly remarkable idea in the chapter.
Every SI base unit is now defined by declaring a constant of nature to be exact. No unit depends on a physical object any more.
| Base quantity | Unit | Symbol | Fixed by declaring |
|---|---|---|---|
| Length | metre | m | speed of light c = 299792458 m/s |
| Mass | kilogram | kg | Planck constant h = 6.62607015 × 10⁻³⁴ J s |
| Time | second | s | caesium-133 frequency Δν = 9192631770 Hz |
| Electric current | ampere | A | elementary charge e = 1.602176634 × 10⁻¹⁹ C |
| Temperature | kelvin | K | Boltzmann constant k = 1.380649 × 10⁻²³ J/K |
| Amount of substance | mole | mol | Avogadro constant Nₐ = 6.02214076 × 10²³ /mol |
| Luminous intensity | candela | cd | luminous efficacy K_cd = 683 lm/W |
You do not need to memorise these numbers. They are quoted only to show how precisely each constant is now known.
Why the kilogram changed
Until 2019 the kilogram was an actual metal cylinder — platinum-iridium, kept in a vault outside Paris.
That is a poor foundation. A physical object can pick up contamination or be damaged. If it drifts, every kilogram on Earth drifts with it.
The fix reverses the logic:
| Old approach | New approach |
|---|---|
| Object defines the unit | Constant defines the unit |
| Realising a kg = compare to the object | Realising a kg = an experiment |
| Only one master copy exists | Any equipped lab can reproduce it |
The metre now depends on the second
Light speed is fixed by definition. So once the caesium clock fixes the second, the metre follows automatically.
The metre is defined in terms of the second — not the other way round.
Two supplementary units
| Unit | For | Defined as | Dimensions |
|---|---|---|---|
| radian (rad) | plane angle | arc ÷ radius | dimensionless |
| steradian (sr) | solid angle | area ÷ radius² | dimensionless |
Both are ratios of like quantities, which is why neither has dimensions.
4. Significant Figures (Textbook 1.3)
What the term means
Every measurement carries uncertainty. The way you write a number should show how well you actually know it.
A significant figure count = all reliably known digits, plus the first uncertain one.
Example. A pendulum period written as 1.62 s:
| Digit | Status |
|---|---|
| 1 | certain |
| 6 | certain |
| 2 | first uncertain digit |
That is three significant figures.
The counting rules
Start from one clean case. 2.308 cm has four significant figures. Now change units:
2.308 cm = 0.02308 m = 23.08 mm = 23080 μm
All four still have four significant figures. Changing units cannot make an instrument sharper.
| Rule | Example | Count |
|---|---|---|
| All non-zero digits count | 2.38 | 3 |
| Zeros between non-zeros count | 6.032 | 4 |
| Leading zeros never count | 0.002308 | 4 |
| Trailing zeros with a decimal point count | 3.500 | 4 |
| Trailing zeros without a decimal point are ambiguous | 12300 | 3 |
The trailing-zero trap
Take a length reported as 4.700 m. Those zeros were written deliberately — otherwise the measurer would have written 4.7 m. So it has four significant figures.
Now convert it:
4.700 m = 470.0 cm = 4700 mm = 0.004700 km
Read 4700 mm on its own and the no-decimal rule gives you two figures. That is wrong. A unit change cannot alter measured precision.
The problem is that a plain integer with trailing zeros is genuinely ambiguous.
The fix: always use scientific notation
Write every measurement as a × 10ᵇ, with 1 ≤ a < 10.
| Form | Significant figures |
|---|---|
4.700 × 10² cm | 4 |
4.700 × 10³ mm | 4 |
4.700 × 10⁻³ km | 4 |
The power of ten carries no significance. Every digit in a is significant. No judgement calls remain.
Order of magnitude
Round a to 1 or 10, and the leftover 10ᵇ is the order of magnitude.
| Quantity | Value | Order |
|---|---|---|
| Earth's diameter | 1.28 × 10⁷ m | 10⁷ |
| Hydrogen atom diameter | 1.06 × 10⁻¹⁰ m | 10⁻¹⁰ |
So Earth is 17 orders of magnitude larger than a hydrogen atom — one checkable sentence from two unwieldy numbers.
Exact numbers
Some numbers are exact by definition or by counting. They have unlimited significant figures and never limit a result.
| Exact number | Where it appears |
|---|---|
| the 2 | d = 2r |
| the 2π | T = 2π√(l/g) |
| the n | dividing by n readings when averaging |
5. Arithmetic With Significant Figures (Textbook 1.3)
Two different rules
This is the most commonly confused pair in the chapter.
| Operation | What you count | Example |
|---|---|---|
| Multiply / divide | fewest significant figures | 5.74 ÷ 1.2 = 4.8 |
| Add / subtract | fewest decimal places | 436.32 + 227.2 = 663.8 |
Why they differ
- Multiplication — each factor's fractional uncertainty carries into the product, so the weakest factor caps the result.
- Addition — what matters is the last trustworthy decimal position. Adding
227.2 gcannot give you a trustworthy hundredths digit, because that input has none.
Worked case. 436.32 g + 227.2 g + 0.301 g = 663.821 g by raw arithmetic.
227.2 has only one decimal place → answer is 663.8 g.
Using the multiplication rule here would give 664 g, which misstates the precision in the other direction.
Subtraction loses figures
0.307 m − 0.304 m = 0.003 m
Both inputs had three significant figures. The answer has one. You cannot write 3.00 × 10⁻³ m — that invents two digits the measurement never had.
Example 1.1 — cube
A cube's side is measured as 7.203 m → 4 significant figures, so both answers round to 4.
| Quantity | Raw value | Reported |
|---|---|---|
Surface area 6a² | 311.299254 m² | 311.3 m² |
Volume a³ | 373.714754 m³ | 373.7 m³ |
Example 1.2 — density
5.74 g occupies 1.2 cm³.
| Input | Significant figures |
|---|---|
mass 5.74 g | 3 |
volume 1.2 cm³ | 2 — limiting |
5.74 ÷ 1.2 = 4.8666… → reported as 4.8 g/cm³.
The extra digits on your calculator are false precision, not extra accuracy.
Rounding when the dropped digit is exactly 5
The convention is round to the nearest even digit.
| Number | Rounds to | Why |
|---|---|---|
2.745 | 2.74 | 4 is already even |
2.735 | 2.74 | 3 is odd, bumps to even 4 |
Both land on 2.74, from opposite sides. That is deliberate, not coincidence.
Never round mid-calculation
Carry one extra digit through intermediate steps.
| Approach | Result |
|---|---|
Round 1/9.58 to 3 figures → 0.104, then invert | 9.62 — drifted |
Keep 0.1044, then invert | 9.58 — correct |
Round twice and the error compounds.
6. Uncertainty in a Calculated Result (Textbook 1.3.3)
This section is examinable. CBSE lists "Determining the uncertainty in result" under Unit I.
Writing a measurement with its uncertainty
A metre scale reading of 16.2 cm carries an uncertainty of one least division, ± 0.1 cm.
That can be written two ways — absolute, or as a percentage:
| Measurement | Absolute form | Percentage form |
|---|---|---|
length l | 16.2 ± 0.1 cm | 16.2 cm ± 0.6% |
breadth b | 10.1 ± 0.1 cm | 10.1 cm ± 1% |
The percentage form is what makes combining errors easy.
Combining errors in a product
Rule: for a product or quotient, the percentage errors add.
Worked, straight from the chapter:
| Step | Working |
|---|---|
| Area | l × b = 16.2 × 10.1 = 163.62 cm² |
| Percentage errors add | 0.6% + 1% = 1.6% |
| Convert back to absolute | 1.6% of 163.62 = 2.6 cm² |
| Raw result | 163.62 ± 2.6 cm² |
| Quoted result | 164 ± 3 cm² |
The final rounding matters. An uncertainty of 2.6 is itself only known roughly, so it is quoted
as 3, and the value is rounded to match — 164, not 163.62.
Relative error depends on the number, not just the digit count
Two masses measured on the same balance, both accurate to ± 0.01 g:
| Measurement | Relative error | Working |
|---|---|---|
1.02 g | ± 1% | 0.01 / 1.02 × 100 |
9.89 g | ± 0.1% | 0.01 / 9.89 × 100 |
Same instrument, same absolute uncertainty — but ten times the relative error on the smaller mass. This is why weighing a small sample on a coarse balance is a bad idea.
Subtraction can destroy significant figures
12.9 g − 7.06 g, both given to three significant figures.
You cannot write 5.84 g. The correct answer is 5.8 g.
Addition and subtraction combine uncertainties by decimal places, not by significant figures — so a result can end up with fewer significant figures than either input started with.
7. Dimensions and Dimensional Analysis (Textbook 1.4 to 1.6)
What dimensions are
Every mechanical quantity reduces to a combination of [M], [L] and [T] raised to powers.
| Quantity | Built from | Dimensional formula |
|---|---|---|
| Volume | length³ | [M⁰L³T⁰] |
| Speed | length ÷ time | [M⁰LT⁻¹] |
| Acceleration | length ÷ time² | [M⁰LT⁻²] |
| Force | mass × acceleration | [MLT⁻²] |
| Energy / Work | force × length | [ML²T⁻²] |
| Mass density | mass ÷ volume | [ML⁻³T⁰] |
Dimensions deliberately discard magnitude. Initial velocity, final velocity and average speed are physically different, but all are [LT⁻¹].
Formula vs equation
| Term | Meaning | Example |
|---|---|---|
| Dimensional formula | the powers themselves | [M⁰LT⁻¹] |
| Dimensional equation | quantity equated to its formula | [v] = [M⁰LT⁻¹] |
The principle of homogeneity
Only quantities with the same dimensions can be added or subtracted.
Adding a velocity to a force is as meaningless as adding three apples to two hours. So every term on both sides of a correct equation must match dimensionally.
Test case: x = x₀ + v₀t + ½at²
| Term | Dimensions |
|---|---|
x | [L] |
x₀ | [L] |
v₀t | [LT⁻¹][T] = [L] |
½at² | [LT⁻²][T²] = [L] |
All four match. The equation passes.
The test runs one way only
Failing it proves an equation wrong. Passing it never proves an equation right.
A bare numerical factor has no dimensions, so a dimensional check simply cannot see it.
Example 1.3 — checking an equation
Check ½mv² = mgh.
| Side | Working | Result |
|---|---|---|
| Left | [M][LT⁻¹]² | [ML²T⁻²] |
| Right | [M][LT⁻²][L] | [ML²T⁻²] |
They match — dimensionally correct.
Example 1.4 — what dimensions can rule out
Five candidate formulas for kinetic energy. True dimension is [ML²T⁻²].
| Candidate | Dimensions | Verdict |
|---|---|---|
K = m²v³ | [M²L³T⁻³] | eliminated |
K = ½mv² | [ML²T⁻²] | survives |
K = ma | [MLT⁻²] | eliminated — that is force |
K = (3/16)mv² | [ML²T⁻²] | survives |
K = ½mv² + ma | mixed | eliminated — illegal sum |
Two survive, and this is the point of the example.
½mv² and (3/16)mv² are dimensionally identical. The method cannot separate them, because it cannot see the numbers ½ and 3/16.
Only the derivation of kinetic energy from the work-energy theorem (Chapter 5) settles it. The answer is ½mv².
Example 1.5 — deriving a relationship
A pendulum's period T may depend on length l, bob mass m, and g.
Step 1. Assume a product form: T = k·lˣ·gʸ·mᶻ, with k dimensionless.
Step 2. Substitute dimensions:
[T¹] = [L]ˣ [LT⁻²]ʸ [M]ᶻ = L⁽ˣ⁺ʸ⁾ T⁻²ʸ Mᶻ
Step 3. Equate powers separately:
| Base | Equation | Solution |
|---|---|---|
| M | z = 0 | z = 0 |
| L | x + y = 0 | x = ½ |
| T | −2y = 1 | y = −½ |
Step 4. Result: T = k√(l/g)
Two things fall out of this:
- Mass drops out entirely (
z = 0). A pendulum's period does not depend on the bob's weight — a real, testable physics result. kcannot be found this way. The full Newtonian derivation givesk = 2π, soT = 2π√(l/g).
Always state that limitation. The derivation is incomplete without it — you have found the form of the relation, not the constant.
What the method can and cannot do
| Good for | Cannot do |
|---|---|
| Sanity-checking a formula fast | Find dimensionless constants (2π, ½) |
| Converting between unit systems | Handle sin, log, eˣ relationships |
| Finding the form of a relation | Separate torque from energy (both [ML²T⁻²]) |
| Up to three independent variables | Four or more unknowns |
8. What Exercises 1.6 and 1.8 Still Assume
These three exercises lean on the removed instrument material. Here is the minimum you need.
| Instrument | Least count | Typical resolution |
|---|---|---|
| Vernier calliper | main-scale division ÷ vernier divisions | 0.05–0.02 mm |
| Screw gauge | pitch ÷ circular-scale divisions | 0.01 mm |
Least count = the smallest change an instrument can actually resolve.
Worked: a screw gauge of pitch 1.0 mm with 100 circular divisions has least count 1.0 ÷ 100 = 0.01 mm.
More divisions do not mean unlimited precision
Past a point, extra markings outrun what the screw itself can resolve. Backlash — slack in the thread — becomes the real limit, not the dial.
Why more readings help
Any single reading carries random scatter in both directions.
Average enough readings and that scatter increasingly cancels. A mean of 100 readings sits closer to the true value than a mean of 5.
That is the whole reasoning behind Exercise 1.8(c).
9. Summary
- A measurement is a comparison against a standard; a number without a unit means nothing.
- Seven SI base units: metre, kilogram, second, ampere, kelvin, mole, candela.
- Since 2018, every base unit is fixed by declaring a constant of nature exact.
- The kilogram left its platinum-iridium cylinder behind; the metre now depends on the second.
- Significant figures = reliable digits + the first uncertain one.
- A change of units never changes the significant-figure count.
- Scientific notation removes all trailing-zero ambiguity.
- Multiply/divide → fewest significant figures. Add/subtract → fewest decimal places.
- Round a dropped 5 to the nearest even digit; never round mid-calculation.
- Dimensions are the powers of [M], [L], [T] that build a quantity.
- Homogeneity: every term in a correct equation shares dimensions.
- A dimensional check can disprove an equation, never prove one.
- Dimensional analysis gives the form of a relation, never its dimensionless constant.
- Still examinable: uncertainty in a result (Textbook 1.3.3) — relative error, and percentage errors adding for a product.
- Not in this chapter: systematic/random error classification, and instruments as a taught topic.
