2.1.2 - SI units, prefixes and graph labels

2.1.2 - SI units, prefixes and graph labels

Physics answers only communicate clearly when the quantity, number and unit travel together. In this lesson you will use the S.I. base quantities named in this specification, build derived units from them, check whether equations are homogeneous, convert prefixes, and label tables and graph axes in a standard exam style. These conventions look small, but they prevent large errors in calculations and practical data.

Base quantities and base units

A physical quantity is something that can be measured. The 2.1.2 list uses S.I. base quantities as the starting point for the units used throughout the specification.

S.I. base quantity

An S.I. base quantity is treated as independent of other physical quantities in the S.I. system. Its unit is a base unit, such as metre for length or second for time.

For this lesson, learn the six base quantities named in the specification:

Base quantityS.I. base unitUnit symbol
masskilogramkg
lengthmetrem
timeseconds
electric currentampereA
thermodynamic temperaturekelvinK
amount of substancemolemol

The symbol is not optional decoration. m\mathrm{m} means metre when it is the unit symbol for length; mol\mathrm{mol} means mole; A\mathrm{A} means ampere. A numerical answer without its unit is usually incomplete because the same number can mean very different things.

There is one boundary detail to keep tidy. The full international S.I. system also has luminous intensity as a base quantity, with unit candela, but this 2.1.2(a) outcome does not list it. In this lesson, answer using the list above.

For this lesson, start with the base units kg, m, s, A, K and mol.

Derived units from base units

Most useful physics units are derived units. They are made by combining base units according to the definition of the quantity or according to an equation.

Derived unit

A derived unit is formed from S.I. base units by multiplication, division and powers. For example, density has unit kgm−3\mathrm{kg} \mathrm{m}^{-3} because it is mass per unit volume.

The specification gives momentum and density as examples in this section. Without teaching the later topics in detail, you can see how their units are built.

QuantityUnit meaningDerived unit
speedlength per timem s−1\mathrm{m}\,\mathrm{s}^{-1}
accelerationspeed per timem s−2\mathrm{m}\,\mathrm{s}^{-2}
momentummass times velocitykg m s−1\mathrm{kg}\,\mathrm{m}\,\mathrm{s}^{-1}
densitymass per volumekgm−3\mathrm{kg} \mathrm{m}^{-3}
forcemass times accelerationkg m s−2\mathrm{kg}\,\mathrm{m}\,\mathrm{s}^{-2}, also called N
pressureforce per areakgm−1s−2\mathrm{kg} \mathrm{m}^{-1} \mathrm{s}^{-2}, also called Pa

The course also uses the following named units. Use the defining relationship to reconstruct them rather than memorising a string of exponents. The later topic lessons explain the physical quantities in detail.

QuantityUnit symbol and useful relationshipSI base-unit expression
Energy/workJ=N m\mathrm{J}=\mathrm{N}\,\mathrm{m}kg m2 s−2\mathrm{kg}\,\mathrm{m}^2\,\mathrm{s}^{-2}
PowerW=J s−1\mathrm{W}=\mathrm{J}\,\mathrm{s}^{-1}kg m2 s−3\mathrm{kg}\,\mathrm{m}^2\,\mathrm{s}^{-3}
FrequencyHz=s−1\mathrm{Hz}=\mathrm{s}^{-1}s−1\mathrm{s}^{-1}
ChargeC=A s\mathrm{C}=\mathrm{A}\,\mathrm{s}A s\mathrm{A}\,\mathrm{s}
Potential differenceV=J C−1\mathrm{V}=\mathrm{J}\,\mathrm{C}^{-1}kg m2 s−3 A−1\mathrm{kg}\,\mathrm{m}^2\,\mathrm{s}^{-3}\,\mathrm{A}^{-1}
ResistanceΩ=V A−1\Omega=\mathrm{V}\,\mathrm{A}^{-1}kg m2 s−3 A−2\mathrm{kg}\,\mathrm{m}^2\,\mathrm{s}^{-3}\,\mathrm{A}^{-2}
CapacitanceF=C V−1\mathrm{F}=\mathrm{C}\,\mathrm{V}^{-1}kg−1 m−2 s4 A2\mathrm{kg}^{-1}\,\mathrm{m}^{-2}\,\mathrm{s}^{4}\,\mathrm{A}^{2}
Magnetic flux densityT=N (A m)−1\mathrm{T}=\mathrm{N}\,(\mathrm{A}\,\mathrm{m})^{-1}kg s−2 A−1\mathrm{kg}\,\mathrm{s}^{-2}\,\mathrm{A}^{-1}
Magnetic fluxWb=T m2\mathrm{Wb}=\mathrm{T}\,\mathrm{m}^{2}kg m2 s−2 A−1\mathrm{kg}\,\mathrm{m}^2\,\mathrm{s}^{-2}\,\mathrm{A}^{-1}
ActivityBq=s−1\mathrm{Bq}=\mathrm{s}^{-1}s−1\mathrm{s}^{-1}

For example, a volt is a joule per coulomb, so divide kg m2 s−2\mathrm{kg}\,\mathrm{m}^2\,\mathrm{s}^{-2} by A s\mathrm{A}\,\mathrm{s}: the extra second in the denominator gives s−3\mathrm{s}^{-3}. Equal base units do not always mean equal physical quantities: hertz describes cycles per second, while becquerel describes decays per second.

The electronvolt (eV) is an energy unit, not a voltage: 1 eV=1.60×10−19 J1\,\mathrm{eV}=1.60\times10^{-19}\,\mathrm{J} using the data-booklet value of elementary charge. The unified atomic mass unit u is a mass unit, 1 u=1.661×10−27 kg1\,\mathrm{u}=1.661\times10^{-27}\,\mathrm{kg}. They are useful non-SI units that must be converted when an equation requires joules or kilograms. Angle in radians is dimensionless because it is arc length divided by radius.

Worked example: deriving a density unit

A material has mass measured in kg and volume measured in m3\mathrm{m}^{3}. Density is mass divided by volume:

ρ=mV\rho = \frac{m}{V}

The unit is therefore:

kgm3=kg m−3\frac{\text{kg}}{\text{m}^3} = \text{kg m}^{-3}

So a density should be written as, for example, 7800 kg m−37800\,\mathrm{kg}\,\mathrm{m}^{-3}, not just 78007800.

Worked example: deriving the newton from base units

The unit of force can be found from the relationship force = mass × acceleration:

unit of force=kg×m s−2\text{unit of force} = \text{kg} \times \text{m s}^{-2}

So:

1 N=1 kg m s−21\ \text{N} = 1\ \text{kg m s}^{-2}

This is the style used when a question asks for a unit in base units.

Checking homogeneity

An equation is homogeneous when every term that is added, subtracted or equated has the same base units. Check this by replacing each quantity with its S.I. base unit expression.

Homogeneous equation

A homogeneous equation has the same base units on both sides. Terms that are added or subtracted must also have the same units as each other.

Homogeneity is a powerful error check. It catches many wrong equations, missing powers and wrong rearrangements before you put numbers into a calculator.

Worked example: checking p=mvp = mv

Suppose pp is momentum, mm is mass and vv is velocity.

Left-hand side:

p has unit kg m s−1p \text{ has unit kg m s}^{-1}

Right-hand side:

mv=kg×m s−1=kg m s−1m v = \text{kg} \times \text{m s}^{-1} = \text{kg m s}^{-1}

Both sides have unit kg m s−1\mathrm{kg}\,\mathrm{m}\,\mathrm{s}^{-1}, so the equation is homogeneous.

Worked example: rejecting a non-homogeneous equation

Someone suggests:

speed=distance×time\text{speed} = \text{distance} \times \text{time}

The left-hand side has unit m s−1\mathrm{m}\,\mathrm{s}^{-1}. The right-hand side has unit:

m×s=m s\text{m} \times \text{s} = \text{m s}

The units do not match, so the equation cannot be correct.

Be careful: homogeneity is necessary, but it is not a complete proof. The equations s=uts = ut and s=2uts = 2ut are both homogeneous because both sides have unit m. Unit checking cannot tell you whether a numerical factor such as 2 is physically correct.

Prefixes and powers of ten

S.I. prefixes are decimal multipliers attached to unit symbols. They make very large and very small values readable.

PrefixSymbolFactor
picop10−1210^{-12}
nanon10−910^{-9}
microμ10−610^{-6}
millim10−310^{-3}
centic10−210^{-2}
decid10−110^{-1}
kilok10310^{3}
megaM10610^{6}
gigaG10910^{9}
teraT101210^{12}

Prefix symbols are case-sensitive. mW\mathrm{mW} is a milliwatt, 10−310^{-3} W. MW\mathrm{MW} is a megawatt, 10610^6 W. Confusing m\mathrm{m} and M\mathrm{M} changes the value by a factor of 10910^9.

The prefix attaches directly to the unit symbol: ms\mathrm{ms} means millisecond, not metre second. In calculations, a safe method is to convert all data to base S.I. units before substituting, unless the equation and answer are deliberately being handled in another consistent unit.

Worked example: ordinary prefix conversion

Convert 4.8 ms4.8\ \text{ms} into seconds.

1 ms=10−3 s1\ \text{ms} = 10^{-3}\ \text{s}

So:

4.8 ms=4.8×10−3 s4.8\ \text{ms} = 4.8 \times 10^{-3}\ \text{s}

Worked example: the squared or cubed prefix trap

Convert 12.0 cm312.0\ \text{cm}^3 into m3\mathrm{m}^{3}.

The prefix is part of the unit being cubed:

1 cm=10−2 m1\ \text{cm} = 10^{-2}\ \text{m}

Therefore:

1 cm3=(10−2 m)3=10−6 m31\ \text{cm}^3 = (10^{-2}\ \text{m})^3 = 10^{-6}\ \text{m}^3

So:

12.0 cm3=12.0×10−6 m3=1.20×10−5 m312.0\ \text{cm}^3 = 12.0 \times 10^{-6}\ \text{m}^3 = 1.20 \times 10^{-5}\ \text{m}^3

The common wrong answer is 12.0×10−2 m312.0 \times 10^{-2}\ \text{m}^3. That treats cm3\mathrm{cm}^{3} as if only the number, not the whole unit, had the prefix.

Graph axes and table columns

Graph axes and table columns should make the quantity and the unit clear. The cleanest convention is:

quantity/unit\text{quantity} / \text{unit}

For example:

  • time/s\text{time} /\mathrm{s}
  • speed/m s−1\text{speed} /\mathrm{m}\,\mathrm{s}^{-1}
  • current/mA\text{current} /\mathrm{mA}
  • temperature/K\text{temperature} /\mathrm{K}
  • density/kg m−3\text{density} /\mathrm{kg}\,\mathrm{m}^{-3}

This means the numbers written in the column or read from the axis are numerical values in that unit. If the axis says current/mA\text{current} /\mathrm{mA}, a plotted value of 12 means 12 mA12\ \text{mA}, which is 12×10−3 A12 \times 10^{-3}\ \text{A}.

Tables follow the same idea. Put the unit in the heading, not repeatedly in the body:

Good headingExample entry
time / s1.20
extension / mm8.5
force / N2.40

Do not write units after every number inside the data cells. That makes data harder to scan and is not good practical style.

For graph axes, a scale factor can also be included in the label. For example:

1/R/10−6Ω−11/R / 10^{-6} \Omega^{-1}

means that the plotted number is the value of 1/R1/R divided by 10−6 Ω−110^{-6}\ \Omega^{-1}. A plotted value of 4.0 corresponds to:

1/R=4.0×10−6 Ω−11/R = 4.0 \times 10^{-6}\ \Omega^{-1}

This convention lets very small or very large values fit neatly onto a graph. It is still your responsibility to carry the scale factor into any calculation involving the gradient, intercept or read-off.

Logarithms are a special case. You can only take the logarithm of a quantity with no units, such as a ratio. A graph label such as ln⁡(V/V0)\ln(V / V_0) is acceptable because V/V0V/V_0 is dimensionless.

Worked example: correcting labels

A student records a table with headings:

tvelocity
0.0 s0.0\,\mathrm{s}0.0 m s−10.0\,\mathrm{m}\,\mathrm{s}^{-1}
0.5 s0.5\,\mathrm{s}1.2 m s−11.2\,\mathrm{m}\,\mathrm{s}^{-1}

A better table is:

time / svelocity / m s−1\mathrm{m}\,\mathrm{s}^{-1}
0.00.0
0.51.2

The improved version states the physical quantity, separates the unit using a solidus, and keeps units out of the body of the table.
[DIAGRAM: asset_slug: units_graph_scale; caption: Current axes in amperes and milliamperes give different numerical gradients but the same resistance of 200 Ω.; description: The same current data shown in amperes and milliamperes: axis scaling changes the numerical slope, while the resistance remains 200 Ω.]
Current axes in amperes and milliamperes give different numerical gradients but the same resistance of 200 Ω.