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Physics · Ch 1 — Units and Measurement

The International System of Units

1.2

The International System of Units

The Need for a Universal System

Before the modern era, scientists in different countries used different systems of units. This created confusion when comparing experimental results across borders. Three older systems were in widespread use:

  • CGS system: centimetre, gram, second
  • FPS (British) system: foot, pound, second
  • MKS system: metre, kilogram, second

The problem is obvious: a measurement of force in the CGS system (dyne) and one in the FPS system (poundal) are not directly comparable without messy conversion factors. What was needed was a single, coherent system that everyone could agree on.

The SI System

The internationally accepted system today is the Système International d'Unités (International System of Units), abbreviated as SI. It was developed by the Bureau International des Poids et Mesures (BIPM) and was originally established in 1971. The most recent major revision came from the General Conference on Weights and Measures in November 2018.

The SI system uses the decimal system, which makes conversions within the system straightforward. For example, converting from metres to kilometres simply means moving the decimal point — no awkward factors like 12 inches to a foot or 3 feet to a yard.

The Seven Base Units

The SI system defines seven base units, each corresponding to a fundamental physical quantity that cannot be expressed in terms of other quantities. These are shown in the table below.

Base QuantityNameSymbol
Lengthmetrem
Masskilogramkg
Timeseconds
Electric currentampereA
Thermodynamic temperaturekelvinK
Amount of substancemolemol
Luminous intensitycandelacd

Each of these units is now defined in terms of fixed numerical values of fundamental physical constants. This is a crucial shift from older definitions that relied on physical artefacts (like the standard metre bar or the standard kilogram cylinder). Constants of nature do not change, so definitions based on them are permanent and universally reproducible.

Definition of the Metre

The metre is defined by fixing the numerical value of the speed of light in vacuum, cc, to be 299 792 458299\,792\,458 when expressed in the unit m s−1\text{m s}^{-1}. The second is itself defined in terms of the caesium frequency ΔνCs\Delta \nu_{\text{Cs}}.

Important

The metre is no longer a fraction of the Earth's meridian or the length of a platinum-iridium bar. It is now derived from the speed of light, a universal constant.

Definition of the Kilogram

The kilogram is defined by fixing the numerical value of the Planck constant hh to be 6.626 070 15×10−346.626\,070\,15 \times 10^{-34} when expressed in the unit J s\text{J s}, which is equivalent to kg m2s−1\text{kg m}^2 \text{s}^{-1}. The metre and the second are themselves defined in terms of cc and ΔνCs\Delta \nu_{\text{Cs}}.

Watch out

The old "international prototype of the kilogram" — a cylinder of platinum-iridium alloy kept in France — is no longer the definition. That artefact's mass was slowly changing due to surface contamination and other effects. The new definition based on the Planck constant is immutable.

Definition of the Second

The second is defined by fixing the numerical value of the caesium frequency ΔνCs\Delta \nu_{\text{Cs}}, which is the unperturbed ground-state hyperfine transition frequency of the caesium-133 atom, to be 9 192 631 7709\,192\,631\,770 when expressed in the unit Hz, which is equivalent to s−1\text{s}^{-1}.

Definition of the Ampere

The ampere is defined by fixing the numerical value of the elementary charge ee to be 1.602 176 634×10−191.602\,176\,634 \times 10^{-19} when expressed in the unit C, which is equivalent to A s\text{A s}. The second is defined in terms of ΔνCs\Delta \nu_{\text{Cs}}.

Definition of the Kelvin

The kelvin is defined by fixing the numerical value of the Boltzmann constant kk to be 1.380 649×10−231.380\,649 \times 10^{-23} when expressed in the unit J K−1\text{J K}^{-1}, which is equivalent to kg m2s−2K−1\text{kg m}^2 \text{s}^{-2} \text{K}^{-1}. The kilogram, metre, and second are defined in terms of hh, cc, and ΔνCs\Delta \nu_{\text{Cs}}.

Definition of the Mole

The mole is defined by fixing the numerical value of the Avogadro constant NAN_A to be 6.022 140 76×10236.022\,140\,76 \times 10^{23} when expressed in the unit mol−1\text{mol}^{-1}. This number is called the Avogadro number. One mole contains exactly this many elementary entities.

Note

When using the mole, the elementary entities must be specified. These can be atoms, molecules, ions, electrons, or any other specified group of particles. Saying "one mole of oxygen" is ambiguous — it could mean one mole of oxygen atoms (O) or one mole of oxygen molecules (O2_2).

Definition of the Candela

The candela is defined by fixing the numerical value of the luminous efficacy of monochromatic radiation of frequency 540×1012540 \times 10^{12} Hz, KcdK_{\text{cd}}, to be 683 when expressed in the unit lm W−1\text{lm W}^{-1}, which is equivalent to cd sr W−1\text{cd sr W}^{-1} or cd sr kg−1m−2s3\text{cd sr kg}^{-1} \text{m}^{-2} \text{s}^3. The kilogram, metre, and second are defined in terms of hh, cc, and ΔνCs\Delta \nu_{\text{Cs}}.

Tip

You are not expected to memorise the exact numerical values in these definitions. They are given to show the extraordinary precision with which modern measurements are made. What matters is understanding the principle: each base unit is now defined by fixing a fundamental constant.

Supplementary Units: Plane Angle and Solid Angle

In addition to the seven base units, the SI defines two supplementary quantities that are dimensionless but have named units.

Plane Angle

A plane angle dθd\theta is defined as the ratio of the length of an arc dsds to the radius rr of the circle:

dθ=dsrd\theta = \frac{ds}{r}

The unit of plane angle is the radian (symbol: rad). Since both dsds and rr have the dimension of length, the ratio is dimensionless.

Solid Angle

A solid angle dΩd\Omega is defined as the ratio of the intercepted area dAdA on a spherical surface to the square of the radius rr:

dΩ=dAr2d\Omega = \frac{dA}{r^2}

The unit of solid angle is the steradian (symbol: sr). Again, since dAdA has dimensions of length squared and r2r^2 has dimensions of length squared, the ratio is dimensionless.

Important

Both the radian and the steradian are dimensionless quantities. They are included in the SI system for convenience when dealing with angular measurements, but they do not add a new fundamental dimension.

Derived Units

All other physical quantities can be expressed in terms of the seven base units. These are called derived units. For example:

  • Speed is length divided by time: m s−1\text{m s}^{-1}
  • Acceleration is speed divided by time: m s−2\text{m s}^{-2}
  • Force is mass times acceleration: kg m s−2\text{kg m s}^{-2}, which is given the special name newton (N)
  • Energy is force times distance: kg m2s−2\text{kg m}^2 \text{s}^{-2}, which is given the special name joule (J)
  • Power is energy per unit time: kg m2s−3\text{kg m}^2 \text{s}^{-3}, which is given the special name watt (W)

A comprehensive list of derived units with special names is provided in the appendices of the textbook.

Units Outside the SI

Some units that are not part of the SI system are still retained for general use because of their widespread acceptance in specific contexts. These are listed in Table 1.2 of the textbook.

Table 1.2 — Some units retained for general use (though outside SI):

NameSymbolValue in SI Unit
minutemin60 s
hourh60 min = 3600 s
dayd24 h = 86400 s
yeary365.25 d = 3.156×1073.156 \times 10^7 s
degree°1°=(π/180)1° = (\pi/180) rad
litreL1 dm3^3 = 10−310^{-3} m3^3
tonnet10310^3 kg
Figure 1.1Description of (a) plane angle dθ, defined as the ratio of the arc length ds to the radius r, and (b) solid angle dΩ, defined as the ratio of the intercepted spherical-surface area dA to the square of the radius r², both described about the apex O as the centre.
Fig. 1.1 — Description of (a) plane angle dθ, defined as the ratio of the arc length ds to the radius r, and (b) solid angle dΩ, defined as the ratio of the intercepted spherical-surface area dA to the square of the radius r², both described about the apex O as the centre.

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

Panel (a) shows the plane angle dθ subtended at a point O by a small arc of length ds on a circle of radius r centred at O: two straight lines (radii) go out from O, an angle dθ opens between them near the vertex, and the arc ds joins their far ends. By the geometric definition of angle in radian measure,

dθ=dsr radiand\theta = \dfrac{ds}{r} \ \text{radian}

Panel (b) extends the same idea to three dimensions. From the apex O, a cone of rays goes out to a small patch of area dA on a sphere of radius r centred at O (the dashed line marks the cone's central axis, running from O to the far side of the patch). The solid angle dΩ is the small 3-D opening at O bounded by that cone, and is defined as the ratio of the intercepted area to the square of the radius:

dΩ=dAr2 steradiand\Omega = \dfrac{dA}{r^{2}} \ \text{steradian} …