Measurements and their Errors

AQA Physics A-Level Study Notes

Section 1: Measurements and their Errors

3.1 Measurements and Their Errors
3.1.1 - Uses of SI Units and Their Prefixes
  • SI Units: The fundamental units used in physics, essential for precise measurement. They comprise:

    • Mass (m): kg (kilograms)

    • Length (l): m (meters)

    • Time (t): s (seconds)

    • Amount of substance (n): mol (moles)

    • Temperature (T): K (kelvin)

    • Electric current (I): A (amperes)

  • Derived Units: The SI units of quantities can be derived from their fundamental forms. For example, the formula for force is given by:

    • F=maF = ma

    • The SI units for force (F) can be determined as:

    • extMass:<br>ightarrowkgext{Mass:} <br>ightarrow kg

    • extAcceleration:<br>ightarrowmexts2ext{Acceleration:} <br>ightarrow m ext{s}^{-2}

    • Thus, the units for force become:

      • kgimesmimess2kg imes m imes s^{-2} (which is also known as N, Newtons)

  • Example of Voltage (V) Calculation: To find the SI units of voltage:

    • Voltage defined as V=racEQV = rac{E}{Q}
      where E is energy and Q is charge.

    • Energy can be expressed as E=rac12mv2E = rac{1}{2}mv^2, thus SI units:

    • For energy: kgimesracm2s2kg imes rac{m^2}{s^2}

    • Charge can be defined as Q=ItQ = It,

    • For charge: AsAs (ampere-seconds)

    • Therefore, simplifying:

      • V=racAskgimesmimess2V = rac{As}{kg imes m imes s^{-2}} gives:

      • V=racAsimess2kgimesm=racAimesskgimesm2V = rac{As imes s^2}{kg imes m} = rac{A imes s}{kg} imes m^2

  • SI Unit Prefixes: Additional prefixes used to denote multiples and submultiples of SI units include:

    • Tera (T): 101210^{12}

    • Giga (G): 10910^{9}

    • Mega (M): 10610^{6}

    • Kilo (k): 10310^{3}

    • Centi (c): 10210^{-2}

    • Milli (m): 10310^{-3}

    • Micro (µ): 10610^{-6}

    • Nano (n): 10910^{-9}

    • Pico (p): 101210^{-12}

    • Femto (f): 101510^{-15}

3.1.2 - Limitation of Physical Measurements
  • Random Errors:

    • Affect the precision of measurements and lead to variations around a mean value.

    • Example: Electronic noise in instruments.

    • To minimize random errors, one should:

    • Take at least three measurements and calculate the mean; this helps identify anomalies.

    • Utilize technology such as computers and data loggers to reduce human error.

    • Employ high-resolution equipment, e.g. a micrometer offers a resolution of 0.1 mm compared to a ruler's 1 mm.

  • Systematic Errors:

    • Impact accuracy and cause consistent deviations in one direction (either high or low).

    • Example: A scale that is not zeroed correctly (zero error) or parallax error when reading scales at an angle.

    • To minimize systematic errors, one might:

    • Calibrate devices against known values (e.g. weighing a 1 kg standard).

    • Correct for background radiation in experiments by measuring it first and excluding from results.

    • Read liquid levels at eye level to avoid parallax errors.

  • Precision

    • Defined as the consistency of measurement, even if they deviate from the actual value.

  • Repeatability

    • The ability for the original experimenter to replicate the experiment with the same setup and obtaining similar results.

  • Reproducibility

    • If another experimenter, using different methods or equipment, achieves the same results.

  • Resolution

    • The smallest distinguishable change in the quantity measured that results in a noticeable change in reading.

  • Accuracy

    • Measures how close a value is to the actual, true value.

  • Uncertainty

    • The extent to which a result may vary, described with bounds, e.g. for a temperature reading of 20°C ± 2°C, where true value could be within 18-22°C.

  • Types of Uncertainty:

    • Absolute Uncertainty: Given as a fixed value, e.g. extVoltage:7.0extVext±0.6Vext{Voltage:} 7.0 ext{ V} ext{ ± 0.6 V}.

    • Fractional Uncertainty: Expressed as a fraction of the measurement, e.g. 7.0extVext±rac0.37extV7.0 ext{ V} ext{ ± } rac{0.3}{7} ext{ V}.

    • Percentage Uncertainty: Given as a percentage of the measurement, e.g. 7.0 ext{ V} ext{ ± } 8.6 ext{%}.

  • Reducing Percentage and Fractional Uncertainty:

    • Measure larger quantities whenever possible.

  • Reading vs. Measuring:

    • Readings involve one value, e.g. temperature from a thermometer.

    • Measurements compare two values, e.g. the difference read from a ruler.

  • Uncertainty Calculation:

    • Uncertainty for a reading is ± half the smallest division.

    • Uncertainty for measurements takes into account both ends. For instance:

    • For a ruler, if each side ±0.5extmm±0.5 ext{ mm}, the total uncertainty is ±1extmm±1 ext{ mm}.

  • Digital Values:

    • Often quoted or assumed as ±± the last significant digit.

  • Reducing Uncertainty Techniques:

    • Fix one end of the measuring device to reduce measured uncertainty.

    • Increase the number of measurements to refine results by averaging. For instance, measuring the time for multiple swings can yield:

    • 10extswings:6.2ext±0.1exts<br>ightarrow1extswing:0.62ext±0.01exts10 ext{ swings: } 6.2 ext{ ± } 0.1 ext{ s} <br>ightarrow 1 ext{ swing: } 0.62 ext{ ± } 0.01 ext{ s}.

  • Significant Figures in Uncertainty:

    • Uncertainties should match the number of significant figures of the data values.

  • Combining Uncertainties:

    • For Addition/Subtraction: Add absolute uncertainties.

    • Example Calculation:

      • If a thermometer shows water temperature dropping from 298ext±0.5K298 ext{ ± 0.5 K} to 273ext±0.5K:273 ext{ ± 0.5 K}:

      • Temperature Difference Calculation:

        • 298273=25K298 - 273 = 25 K

        • Total Uncertainty: 0.5+0.5=1K0.5 + 0.5 = 1 K

        • Final Difference: 25ext±1K25 ext{ ± } 1 K

  • For Multiplying/Dividing: Add percentage uncertainties.

    • Example Problem:

      • Given force of 91ext±3N91 ext{ ± 3 N} and mass of 7ext±0.2kg7 ext{ ± 0.2 kg}:

      • Acceleration Calculation: a=racFm=rac917=13extms2a = rac{F}{m} = rac{91}{7} = 13 ext{ m s}^{-2}

      • Calculate percentage uncertainty:

        • Uncertainty % = rac{3}{91} imes 100 = 3.3 ext{%}

        • Uncertainty % for mass = rac{0.2}{7} imes 100 = 2.9 ext{%}

        • Total = 3.3 ext{%} + 2.9 ext{%} = 6.2 ext{%}

        • Thus, a=13ext±0.8ms2a = 13 ext{ ± } 0.8 m s^{-2} where 6.2 ext{%} ext{ of } 13 ext{ is } 0.8.

  • Raising Measurements to a Power: Multiply percentage uncertainty by the power raised.

    • Example Problem:

      • For a circle with radius 5ext±0.3cm5 ext{ ± 0.3 cm}, percentage uncertainty in area:

      • Area formula: A=extπr2A = ext{π} r^2 thus:

        • Area Calculation: A=extπimes25=78.5extcm2A = ext{π} imes 25 = 78.5 ext{ cm}^2.

        • % uncertainty in radius = rac{0.3}{5} imes 100 = 6 ext{%}.

        • % uncertainty in area = 6 ext{%} imes 2 = 12 ext{%}.

        • Final Area with Uncertainty: A = 78.5 ext{ ± } 12 ext{%} ext{ cm}^2.

  • Uncertainties on Graphs:

    • Represent uncertainties via error bars. E.g., if uncertainty = 5 mm, represent with 5 squares error bar on either side of a data point.

    • A line of best fit must pass through all error bars, neglecting any anomalous points.

    • Gradient uncertainties: Calculated using the steepest and shallowest lines of worst fit that cover all error bars.

    • Gradient Uncertainty Calculation:

      • ext{Percentage Uncertainty} = rac{ ext{Best Gradient}}{100 ext{%}} imes | ext{Best Gradient} - ext{Worst Gradient}|.

3.1.3 - Estimation of Physical Quantities
  • Orders of Magnitude:

    • Powers of ten indicating the scale of an object, useful for comparing sizes.

    • Example: Diameter of atomic nuclei is around 1014m10^{-14} m.

    • Comparison: 100m100 m is two orders of magnitude greater than 1m1 m.

    • Nearest Order of Magnitude Calculation:

    • For diameter of a hydrogen atom, find approximate area assuming a spherical shape:

    • extDiameter=1.06imes1010mext{Diameter} = 1.06 imes 10^{-10} m, thus radius r=0.53imes1010mr = 0.53 imes 10^{-10} m.

    • Use the area formula:

      • A=extπr2=extπimes(0.53imes1010)2=extπimes2.8imes1021m2A = ext{π}r^2 = ext{π} imes (0.53 imes 10^{-10})^2 = ext{π} imes 2.8 imes 10^{-21} m^2,

      • Resulting area approximated to 8imes1021m28 imes 10^{-21} m^2 (expressed to 1 s.f.).

    • Final answer rounded to nearest order of magnitude: 1020m210^{-20} m^2.

  • Estimation in Physics:

    • Necessary to approximate physical quantities for comparisons or validation of calculated values.