Processing data in Physics (DP IB Physics): Revision Note

Katie M

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Katie M

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Processing data in Physics

  • This is the "calculation" phase of your investigation

  • Data processing involves applying mathematical calculations to your raw data to determine the final values you need to answer your research question

    • For example, calculating a period, a resistance, or an acceleration due to gravity

Principles of data processing

Carry out relevant and accurate data processing

  • The goal of data processing is to carry out relevant and accurate calculations to transform raw data into a form which is easier to interpret

    • This involves calculating mean values, propagating uncertainties, and presenting the results clearly

  • Show your working clearly

    • For every type of calculation you perform, you must show one full, worked example

  • Calculating an average

    • When you have repeat trials, you must calculate an average (mean) value to use in further calculations

    • You should exclude any anomalous results from your average

  • Propagating uncertainties

    • The uncertainties from your raw measurements must be carried through your calculations to find the uncertainty in your final, processed result

    • For addition or subtraction, add the absolute uncertainties.

      • Example: To find the length L of an object, you measure final position - initial position on a ruler

      • The uncertainty in L is (uncertainty of final position) + (uncertainty of initial position)

      • For a ruler, this is 0.5 mm + 0.5 mm = 1 mm

    • For multiplication or division, add the fractional or percentage uncertainties.

      • Example: To determine the resistance R of a component, you would measure potential difference V and current I and calculate using R space equals space V over I

      • The % uncertainty in R is (% uncertainty in V) + (% uncertainty in I)

    • For quantities that are raised to a power, multiply the fractional or percentage uncertainty by the power

      • Example: To determine the kinetic energy E subscript k of an object, you would measure mass m and speed v and calculate using E subscript k space equals space 1 half m v squared

      • The % uncertainty in E subscript k is (% uncertainty in m) + 2×(% uncertainty in v)

  • Significant figures

    • Your final calculated answer should be given to a number of significant figures that reflects the precision of the raw data used

      • The general rule is that your final answer should have the same number of significant figures as the least precise piece of data used in the calculation

Presenting data in tables

  • Your processed data should be presented in a neat, clearly labelled table

    • It is good practice to show the raw data and processed data in the same table

  • Tables must include:

    • a descriptive numbered title

      • For example, "Table 1: Time taken for 20 swings of varying lengths of a pendulum"

    • appropriate column headers

      • For each variable, include the name of the quantity, the unit of measurement, and the absolute uncertainty (using the ± symbol)

      • The independent variable should be in the first column, followed by the dependent variables in subsequent columns

    • all the raw and processed data

      • For each variable, all recorded data should have the same number of decimal places

      • The number of significant figures used for the data should also be consistent with the quoted uncertainties

Presenting data graphically

  • A graph is the most powerful tool for representing your results

    • It turns lists of numbers into a clear visual pattern

  • A correctly formatted scientific graph must include:

    • a descriptive title

      • For example, "A graph to show the relationship between the period squared and the length of a simple pendulum"

    • labelled axes with units

      • The independent variable is plotted on the x-axis

      • The dependent variable is plotted on the y-axis

    • an appropriate scale

      • Both axes should begin at the origin (0, 0), but if not, you should justify why

      • The scale should be chosen so that plotted points take up at least half of the space

    • clearly plotted data points

      • These should be small crosses or points

      • If using points, drawing a circle around them can ensure they are not missed

    • error bars

      • These represent the absolute uncertainty in the measurements

      • If the uncertainty is too small to show as an error bar on a graph, then it may be omitted

    • a line (or curve) of best fit

      • This shows the overall trend in the data

      • This line does not have to go through every single point, but it must go through all the error bars

Linearisation

  • Many relationships in physics are not linear, resulting in a curve when plotted.

  • It is difficult to determine the exact relationship from a curve, so we linearise the data.

  • This involves manipulating the data based on a known physical formula so that it produces a straight line when plotted.

    • For example, the formula for a pendulum is T = 2π√(L/g).

    • This can be rearranged to T2 = (4π2/g)L

    • This is in the form of a straight-line equation, y = mx + c.

    • By plotting T2 (y-axis) against L (x-axis), you should get a straight line through the origin with a gradient (m) equal to 4π2/g.

Worked Example

Research question:

  • "What is the relationship between the length of a simple pendulum and its period of oscillation?"

Raw data for a pendulum length of 0.600 m:

  • Time for 20 oscillations (s): 31.1, 31.2, 31.0

Processing the data:

  1. Calculate the average time for 20 oscillations:

    • Average time t subscript 20 space equals space fraction numerator open parentheses 31.1 plus 31.2 plus 31.0 close parentheses over denominator 3 end fraction = 31.1 s

  2. Calculate the period T of one oscillation:

    • Period T space equals space fraction numerator average space time over denominator 20 end fraction

    • Period T space equals space fraction numerator 31.1 over denominator 20 end fraction = 1.555 s

    • The raw times have 3 s.f., so the period should be 1.56 s

  3. Propagate the uncertainty:

    • The uncertainty in the stopwatch reading was ±0.2 s

    • Percentage uncertainty = fraction numerator absolute space uncertainty over denominator measured space value end fraction× 100

      • % uncertainty in t subscript 20 space equals space fraction numerator 0.2 over denominator 31.1 end fraction × 100 = 0.643%

    • Since T thin space equals space t subscript 20 over 20 (and 20 is an exact number with no uncertainty), the percentage uncertainty in T is the same as in t20

      • So, % uncertainty in T = 0.643%

    • Absolute uncertainty in T = fraction numerator 0.643 over denominator 100 end fraction × 1.555 = 0.01 s (to 1 s.f.)

    • The final period should be quoted to the same number of decimal places as the uncertainty.

      • Final processed result: T = 1.56 ± 0.01 s

Worked Example

Research question:

  • "What is the resistance of a 0.500 m length of constantan wire?"

Raw data for one trial at a length of 0.500 m:

  • Potential difference V = 2.24 ± 0.01 V

  • Current I = 1.51 ± 0.01 A

Processing the data:

  1. Calculate the resistance:

    • R space equals space V over I space equals space fraction numerator 2.24 over denominator 1.51 end fraction = 1.4834 Ω

    • Both V and I are given to 3 s.f., so the final answer should also be to 3 s.f.

    • Resistance R = 1.48 Ω

  2. Propagate the uncertainty:

    • First, find the percentage uncertainty for V and I

      • % uncertainty in V space equals space fraction numerator 0.01 over denominator 2.24 end fraction × 100 = 0.446%

      • % uncertainty in I space equals space fraction numerator 0.01 over denominator 1.51 end fraction × 100 = 0.662%

    • Add the percentage uncertainties to find the percentage uncertainty in R

      • % uncertainty in R = 0.446% + 0.662% = 1.108%

    • Absolute uncertainty in R space equals space fraction numerator 1.108 over denominator 100 end fraction × 1.4834 Ω = 0.0164 Ω

      • The uncertainty should be given to one significant figure: 0.02 Ω

    • The final resistance should be quoted to the same number of decimal places as the uncertainty.

      • Final processed result: R = 1.48 ± 0.02 Ω

Examiner Tips and Tricks

  • Show one full worked example.

    • Even if you use a spreadsheet, you must show the assessor how you got from your raw data to your processed data for one set of values.

    • This is essential for gaining full marks.

  • Watch your significant figures.

    • A common error is to write down the full calculator display.

    • Processed data should not have more significant figures than the raw data used to calculate it.

  • The independent variable always goes on the x-axis.

    • A simple but crucial convention for scientific graphs is that the independent variable is plotted on the horizontal (x) axis, and the dependent variable is on the vertical (y) axis.

  • A line of best fit is not "dot-to-dot".

    • It is a single, straight line or smooth curve that represents the overall trend of your data.

    • It should have roughly the same number of points on either side of it.

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Katie M

Author: Katie M

Expertise: Physics Content Creator

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.