This MCQ module is based on: Errors in Measurement
Errors in Measurement
This assessment will be based on: Errors in Measurement
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Errors in Measurement
Errors in Measurement
No measurement is perfectly accurate. Every measured value differs from the true value by some amount called the error. Understanding errors is crucial because it tells us how much confidence we can place in our results.
Types of Errors
| Error Type | Description | Example |
|---|---|---|
| Systematic Errors | Errors that consistently shift measurements in one direction (always too high or always too low). They have a definite cause. | A zero-error in a vernier caliper; a thermometer that always reads 2°C too high. |
| Random Errors | Errors that fluctuate unpredictably from measurement to measurement due to unknown or uncontrollable factors. | Slight variations in reaction time when using a stopwatch; fluctuations due to small air currents. |
| Least Count Error | The smallest measurement possible with a given instrument. It sets the minimum uncertainty. | A metre ruler with mm markings has a least count of 1 mm; readings are uncertain by ±0.5 mm. |
(i) Instrumental errors — arise from faulty calibration or defects in the instrument.
(ii) Personal errors — arise from the observer's habits (parallax, bias in reading).
(iii) Environmental errors — arise from external conditions (temperature, humidity, vibrations).
Absolute Error, Relative Error, and Percentage Error
Suppose a physical quantity is measured \(n\) times, yielding values \(a_1, a_2, a_3, \ldots, a_n\). The arithmetic mean (best estimate of the true value) is:
Absolute Error
The absolute error in each measurement is the magnitude of the difference between the individual measurement and the mean:
Mean Absolute Error
The average of all the absolute errors gives the mean absolute error:
The measurement is then reported as: \(a = \bar{a} \pm \Delta\bar{a}\)
Relative Error and Percentage Error
Worked Examples — Error Analysis
Example 1: Complete Error Analysis from Repeated Measurements
The diameter of a wire is measured five times with a screw gauge. The readings are: 3.11 mm, 3.15 mm, 3.14 mm, 3.12 mm, 3.16 mm. Find the mean, absolute errors, mean absolute error, relative error, and percentage error.
\[\bar{d} = \frac{3.11 + 3.15 + 3.14 + 3.12 + 3.16}{5} = \frac{15.68}{5} = 3.136 \text{ mm}\] Rounding to 2 decimal places: \(\bar{d} = 3.14\) mm.
Step 2: Calculate absolute errors
\[\begin{aligned} |\Delta d_1| &= |3.11 - 3.14| = 0.03 \text{ mm}\\ |\Delta d_2| &= |3.15 - 3.14| = 0.01 \text{ mm}\\ |\Delta d_3| &= |3.14 - 3.14| = 0.00 \text{ mm}\\ |\Delta d_4| &= |3.12 - 3.14| = 0.02 \text{ mm}\\ |\Delta d_5| &= |3.16 - 3.14| = 0.02 \text{ mm} \end{aligned}\] Step 3: Mean absolute error
\[\Delta\bar{d} = \frac{0.03 + 0.01 + 0.00 + 0.02 + 0.02}{5} = \frac{0.08}{5} = 0.016 \approx 0.02 \text{ mm}\] Step 4: Relative error
\[\frac{\Delta\bar{d}}{\bar{d}} = \frac{0.02}{3.14} = 0.0064\] Step 5: Percentage error
\[\frac{\Delta\bar{d}}{\bar{d}} \times 100\% = 0.0064 \times 100\% = \boxed{0.64\%}\] Result: The diameter is \(d = 3.14 \pm 0.02\) mm with a percentage error of 0.64%.
Combination of Errors
When we compute a derived quantity from measured values, how do the individual errors combine? The rules depend on whether the quantities are added, multiplied, or raised to powers.
Error in Sum or Difference
If \(Z = A + B\) or \(Z = A - B\), then the maximum absolute error in \(Z\) is:
Error in Product or Quotient
If \(Z = A \times B\) or \(Z = \frac{A}{B}\), then the maximum relative error in \(Z\) is:
Error in a Quantity Raised to a Power
If \(Z = A^n\), then:
General Rule for Combined Errors
For a general formula \(Z = \dfrac{A^p \cdot B^q}{C^r}\), the maximum fractional (relative) error is:
Example 2: Error in Period Measurement
A student measures the total time for 20 oscillations of a pendulum as \(t = 39.6 \pm 0.2\) s. What is the percentage error in the time period \(T\)?
The time period \(T = \frac{t}{n}\), where \(n = 20\) (exact number, no error).
\[T = \frac{39.6}{20} = 1.98 \text{ s}\] \[\Delta T = \frac{\Delta t}{n} = \frac{0.2}{20} = 0.01 \text{ s}\] \[\text{Percentage error in } T = \frac{\Delta T}{T} \times 100\% = \frac{0.01}{1.98} \times 100\% = \boxed{0.51\%}\]
Example 3: Error in Density (Product/Quotient of Powers)
The density of a material is calculated using \(\rho = \frac{M}{\pi r^2 L}\). If the percentage errors in measuring \(M\), \(r\), and \(L\) are 1%, 0.5%, and 2% respectively, find the maximum percentage error in \(\rho\).
\[\rho = \frac{M}{\pi r^2 L}\] Taking the general error formula: \(\frac{\Delta\rho}{\rho} = \frac{\Delta M}{M} + 2\frac{\Delta r}{r} + \frac{\Delta L}{L}\)
(Note: \(\pi\) is exact, so no error from it. The power of \(r\) is 2, so its error is multiplied by 2.)
\[\frac{\Delta\rho}{\rho} \times 100\% = 1\% + 2(0.5\%) + 2\% = 1\% + 1\% + 2\% = \boxed{4\%}\]
Example 4: Error in a Complex Expression
A physical quantity \(X\) is related to other measurable quantities by: \(X = \frac{a^2 b^3}{c\sqrt{d}}\). If the percentage errors in \(a, b, c, d\) are 1%, 2%, 3%, and 4% respectively, find the percentage error in \(X\).
Rewriting: \(X = a^2 \cdot b^3 \cdot c^{-1} \cdot d^{-1/2}\)
Applying the general formula:
\[\frac{\Delta X}{X} \times 100\% = 2\left(\frac{\Delta a}{a}\right) + 3\left(\frac{\Delta b}{b}\right) + 1\left(\frac{\Delta c}{c}\right) + \frac{1}{2}\left(\frac{\Delta d}{d}\right)\] \[= 2(1\%) + 3(2\%) + 1(3\%) + \frac{1}{2}(4\%)\] \[= 2\% + 6\% + 3\% + 2\% = \boxed{13\%}\]
Example 5: Error in Resistance
In an experiment, the resistance \(R\) is determined from \(V = IR\), i.e. \(R = V/I\). If \(V = 100 \pm 5\) V and \(I = 10 \pm 0.2\) A, find the percentage error in \(R\) and express the result.
\[R = \frac{V}{I} = \frac{100}{10} = 10\;\Omega\] Percentage error in \(V\): \(\frac{5}{100}\times 100\% = 5\%\)
Percentage error in \(I\): \(\frac{0.2}{10}\times 100\% = 2\%\)
For a quotient: \(\frac{\Delta R}{R}\times 100\% = 5\% + 2\% = 7\%\)
\(\Delta R = 7\% \text{ of } 10 = 0.7\;\Omega\)
\[\boxed{R = 10 \pm 0.7\;\Omega \quad\text{(percentage error = 7\%)}}\]
Accuracy vs Precision
Accuracy and precision are two distinct concepts that are often confused:
- Accuracy refers to how close a measured value is to the true value.
- Precision refers to how close repeated measurements are to each other.
A helpful analogy is target shooting. Imagine four different scenarios:
- Set up a simple pendulum of known length (say, 1 m).
- Calculate the expected period using \(T = 2\pi\sqrt{l/g}\) (theoretical value).
- Measure the time for 20 oscillations using a digital stopwatch. Repeat 5 times.
- Compute the mean, absolute errors, and percentage error.
- Compare your mean value with the theoretical value to assess accuracy.
- Look at how close your 5 readings are to each other to assess precision.
For \(l = 1\) m: \(T_{\text{theory}} = 2\pi\sqrt{1/9.8} \approx 2.007\) s.
If your mean is close to 2.01 s, your measurement is accurate.
If all 5 readings are within 0.02 s of each other, your measurement is precise.
If the mean is, say, 2.10 s (consistently off), you likely have a systematic error — perhaps in measuring the length, or in the reaction time being biased.
Interactive: Error Calculator L3 Apply
Enter up to 5 repeated measurements and compute the error analysis automatically:
Competency-Based Questions
Q1. L1 Remember Define absolute error and relative error.
Q2. L3 Apply Using the five readings given above, calculate the mean radius, mean absolute error, and percentage error in the radius measurement. (3 marks)
Mean: \(\bar{r} = \frac{2.15+2.13+2.14+2.16+2.12}{5} = \frac{10.70}{5} = 2.14\) cm
Absolute errors: |0.01|, |0.01|, |0.00|, |0.02|, |0.02| cm
Mean absolute error: \(\Delta\bar{r} = \frac{0.01+0.01+0.00+0.02+0.02}{5} = \frac{0.06}{5} = 0.012 \approx 0.01\) cm
Percentage error: \(\frac{0.01}{2.14}\times 100\% = 0.47\%\)
Q3. L3 Apply The volume of a sphere is \(V = \frac{4}{3}\pi r^3\). What is the percentage error in the volume? (2 marks)
Since \(V \propto r^3\), the percentage error in \(V\) is:
\[\frac{\Delta V}{V}\times 100\% = 3 \times \frac{\Delta r}{r}\times 100\% = 3 \times 0.47\% = \boxed{1.41\%}\] The power of \(r\) is 3, so the error is magnified threefold.
Q4. L4 Analyse A student finds that when using Instrument A, the measurements are 5.10, 5.11, 5.09, 5.10, 5.10 g. With Instrument B: 5.00, 5.20, 4.90, 5.15, 4.95 g. Both instruments are measuring the same object whose true mass is 5.10 g. Compare the accuracy and precision of the two instruments. (3 marks)
Instrument A: Mean = 5.10 g (equals true value, so high accuracy). Readings vary by at most 0.01 g (high precision).
Instrument B: Mean = \(\frac{5.00+5.20+4.90+5.15+4.95}{5} = 5.04\) g (differs from true value by 0.06 g, so lower accuracy). Readings vary by up to 0.30 g (low precision).
Conclusion: Instrument A is both more accurate and more precise than Instrument B.
Q5. L5 Evaluate A student claims: "Since systematic errors always push measurements in one direction, taking more readings and averaging will eliminate systematic errors." Is this claim correct? Justify your answer. (3 marks)
Assertion-Reason Questions
Assertion (A): When two physical quantities are multiplied, the percentage error in the result is the sum of the individual percentage errors.
Reason (R): Errors always add up to give the maximum possible error in the result.
Assertion (A): The error in a quantity raised to a power is multiplied by that power.
Reason (R): If \(Z = A^n\), then \(\frac{\Delta Z}{Z} = n\frac{\Delta A}{A}\).
Assertion (A): A measurement can be precise without being accurate.
Reason (R): Precision depends on random errors while accuracy depends on systematic errors.