Physical Quantities

Base Quantity

Physical QuantitiesSI UnitSymbolDerived Quantityderived SI units
lengthmetremmaream2\text{m}^2
masskilogramkgkgvolumem3\text{m}^3
timesecondsssspeedm/s\text{m/s}
currentampereAAforceN\text{N}
temperaturekelvinKKpressureN/m2\text{N/m}^2
luminous intensitycandelacdcdpowerW\text{W}
amount of substancemolemolmoldensitykg/m3\text{kg/m}^3
Submultiples<<Multiples<<
FactorPrefixSymbolFactorPrefixSymbol
10−110^{-1}deci-d10110^1deca-da
10−210^{-2}centi-c10210^2hecto-h
10−310^{-3}milli-m10310^3kilo-k
10−610^{-6}micro-μ\mu10610^6mega-M
10−910^{-9}nano-n10910^9giga-G
10−1210^{-12}pico-p101210^{12}tera-T
10−1510^{-15}femto-f101510^{15}peta-P
10−1810^{-18}atto-a101810^{18}exa-E

Measurements

Instruments

InstrumentMaximum MeasurementAccuracy
Metre Rule100cm / 1m0.1cm / 0.001m
Digital Callipers200mm / 0.2m0.01cm / 0.0001m
Digital Micrometre25mm / 0.025m0.001cm / 0.00001m

Accuracy & Precision

IMG-20260403230430355

Errors

systematicrandom
mistakes in experimental designunavoidable but can me minimised
zero error / constant parallax errorlarger sample size / take average of readings

systematic error

  • zero error of the vernier calipers / micrometer used
  • end error of metre rule
  • parallax error in the measurement if observer consistently reads from the same wrong position
  • human reaction time if the observer consistently stops 1 s before pendulum reaches fiducial line

random error

random errors are inherent in the measurement.

  • varying human reaction time which affects the measurement of timing for the determination of the period
  • energy transferred to the environment which affects the measurement of temp. of water
  • parallax error in determining the alignment of pins which affects the measurement of the angle of refraction

sources of error

measuring tape / metre rule

  • parallax error
    • position eyes vertically above the reading of the scale ⇒ line of sight is perpendicular to the rule
    • place the rule such that its scale at the edge is touching / as close to the object to be measured
    • use a thin ruler so that the scale at the edge is touching the object.
  • end error
    • do not use the ends of the rule for any measurements. ⇒ avoid end errors (can occur due to wear and tear of the rule) digital caliper + micrometer
  • application of excessive measuring force → jaws tilt
  • thermal expansion ← temperature difference between caliper + object
  • abbe error (caliper only) — axis of the instrument and the axis along which the object is measured is not aligned

reducing error

random error

  • take multiple readings and find the average of the readings

best fit line

  • the line of best fit has an equal number of readings on both sides
  • ⇒ cancelling out the errors which cause over– and underestimation of the true value
  • ⇒ reducing the effect of the errors on trends

Significant Figures (s.f.)

Sf indicate the precision of a measurement. The more significant figures a number has, the more precise the measurement is.

Rules for Counting Significant Figures

RuleExampleNumber of s.f.
Non-zero digits are always significant.2.32
Zeros after a decimal point (trailing zeros) are always significant.0.5003
Zeros between 2 s.f. (sandwiched zeros) are always significant.7.063
Zeros before a non-zero digit (leading zeros) are not significant.0.0031

Calculations with Significant Figures

  • Multiplication/Division
    • Round final answer to the lowest number of significant figures found in any of the original numbers used in the calculation 4.56(3 s.f.)×1.4(2 s.f.)=6.4(to 2 s.f.)4.56 (\text{3 s.f.}) × 1.4 (\text{2 s.f.}) = 6.4(\text{to 2 s.f.})
  • Addition/subtration
    • Round final answer to the lowest number of decimal places found in the original numbers 12.11(2 d.p.)+18.0(1 d.p.)+1.013(3 d.p.)=31.1(to 3d.p.)12.11 (\text{2 d.p.}) + 18.0 (\text{1 d.p.}) + 1.013 \text{(3 d.p.)} = 31.1\text{(to 3d.p.)}
  • Intermediate working is always to +1 sf/dp
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