Skip to main content

Measurement and Data Processing — Diagnostic Tests

Unit Tests

UT-1: Uncertainty Propagation

Question: The density of a metal cylinder is determined by measuring its mass (m=12.45±0.01 gm = 12.45 \pm 0.01\ \text{g}) and dimensions: diameter (d=1.25±0.01 cmd = 1.25 \pm 0.01\ \text{cm}) and height (h=5.00±0.01 cmh = 5.00 \pm 0.01\ \text{cm}). Calculate the density and its absolute uncertainty. The volume of a cylinder is V=πd2h/4V = \pi d^2 h / 4.

Solution:

V=π×1.252×5.004=π×1.5625×5.004=24.544=6.135 cm3V = \frac{\pi \times 1.25^2 \times 5.00}{4} = \frac{\pi \times 1.5625 \times 5.00}{4} = \frac{24.54}{4} = 6.135\ \text{cm}^3

ρ=mV=12.456.135=2.029 g cm3\rho = \frac{m}{V} = \frac{12.45}{6.135} = 2.029\ \text{g cm}^{-3}

Fractional uncertainty in dd: 0.011.25=0.0080\frac{0.01}{1.25} = 0.0080 (0.80%). Since d2d^2 appears, its contribution is 2×0.0080=0.0162 \times 0.0080 = 0.016 (1.6%).

Fractional uncertainty in hh: 0.015.00=0.0020\frac{0.01}{5.00} = 0.0020 (0.20%).

Fractional uncertainty in mm: 0.0112.45=0.00080\frac{0.01}{12.45} = 0.00080 (0.08%).

Total fractional uncertainty in ρ\rho: (0.016)2+(0.0020)2+(0.00080)2=0.000256+0.000004+0.00000064=0.000261=0.0161\sqrt{(0.016)^2 + (0.0020)^2 + (0.00080)^2} = \sqrt{0.000256 + 0.000004 + 0.00000064} = \sqrt{0.000261} = 0.0161 (1.6%).

Absolute uncertainty: Δρ=2.029×0.0161=0.033 g cm3\Delta\rho = 2.029 \times 0.0161 = 0.033\ \text{g cm}^{-3}.

ρ=2.03±0.03 g cm3\rho = 2.03 \pm 0.03\ \text{g cm}^{-3} (uncertainty given to 1 s.f., value rounded to match).

The diameter measurement dominates the uncertainty because of the d2d^2 term.


UT-2: Significant Figures in Calculations

Question: A student records the following data and performs calculations. Identify and correct all significant figure errors: (a) 0.0250×4.00=0.10000.0250 \times 4.00 = 0.1000, (b) 12.4/3.2=3.87512.4 / 3.2 = 3.875, (c) log(2.5×103)=2.6021\log(2.5 \times 10^{-3}) = -2.6021, (d) The pH is measured as 3.45. Calculate [H+]=103.45=3.548×104[\text{H}^+] = 10^{-3.45} = 3.548 \times 10^{-4}.

Solution:

(a) 0.0250×4.00=0.1000.0250 \times 4.00 = 0.100. Rule: in multiplication, the answer has the same number of significant figures as the factor with the fewest. 0.02500.0250 has 3 s.f., 4.004.00 has 3 s.f. Answer should be 3 s.f.: 0.1000.100. (The student wrote 0.1000 which is 4 s.f. -- incorrect.)

(b) 12.4/3.2=3.912.4 / 3.2 = 3.9. 12.412.4 has 3 s.f., 3.23.2 has 2 s.f. Answer should be 2 s.f.: 3.93.9 (not 3.875).

(c) log(2.5×103)=2.60\log(2.5 \times 10^{-3}) = -2.60. When taking a logarithm, the number of decimal places in the answer equals the number of significant figures in the original. 2.5×1032.5 \times 10^{-3} has 2 s.f., so the log should have 2 decimal places: 2.60-2.60 (not 2.6021-2.6021).

(d) [H+]=103.45=3.5×104[\text{H}^+] = 10^{-3.45} = 3.5 \times 10^{-4}. When taking an antilogarithm, the number of significant figures in the answer equals the number of decimal places in the original. pH =3.45= 3.45 has 2 decimal places, so [H+][\text{H}^+] should have 2 s.f.: 3.5×104 mol dm33.5 \times 10^{-4}\ \text{mol dm}^{-3} (not 3.548×1043.548 \times 10^{-4}).


UT-3: Graphical Analysis and Best-Fit Line

Question: In an experiment to determine the molar mass of an unknown gas, a student measures the mass of gas at different pressures (constant TT, VV). The data should follow m=PMVRTm = \frac{PMV}{RT}. The student plots mm vs PP and obtains a gradient of 0.0445 g kPa10.0445\ \text{g kPa}^{-1}. If V=250 cm3V = 250\ \text{cm}^3 and T=298 KT = 298\ \text{K}, calculate the molar mass. Identify whether the student should force the line through the origin and explain why.

Solution:

From m=MVRT×Pm = \frac{MV}{RT} \times P, the gradient of mm vs PP is MVRT\frac{MV}{RT}.

M=gradient×RTVM = \frac{\text{gradient} \times RT}{V}

Convert units: V=250 cm3=250×106 m3=2.50×104 m3V = 250\ \text{cm}^3 = 250 \times 10^{-6}\ \text{m}^3 = 2.50 \times 10^{-4}\ \text{m}^3. PP in kPa, so R=8.314 J K1mol1R = 8.314\ \text{J K}^{-1}\text{mol}^{-1} and we need gradient in kg Pa1\text{kg Pa}^{-1}:

Gradient =0.0445 g kPa1=4.45×105 kg Pa1= 0.0445\ \text{g kPa}^{-1} = 4.45 \times 10^{-5}\ \text{kg Pa}^{-1}.

M=4.45×105×8.314×2982.50×104=0.11032.50×104=441 g mol1M = \frac{4.45 \times 10^{-5} \times 8.314 \times 298}{2.50 \times 10^{-4}} = \frac{0.1103}{2.50 \times 10^{-4}} = 441\ \text{g mol}^{-1}

(Checking: CO2\text{CO}_2 is 44 g mol144\ \text{g mol}^{-1}, so this is likely CO2\text{CO}_2 with a unit issue. Rechecking: gradient should be 0.0445 g kPa10.0445\ \text{g kPa}^{-1}. Using R=8.314 J K1mol1=8.314×103 kJ K1mol1R = 8.314\ \text{J K}^{-1}\text{mol}^{-1} = 8.314 \times 10^{-3}\ \text{kJ K}^{-1}\text{mol}^{-1} but with pressure in kPa and volume in dm3^3: V=0.250 dm3V = 0.250\ \text{dm}^3.)

M=0.0445×8.314×2980.250=110.30.250=44.1 g mol1M = \frac{0.0445 \times 8.314 \times 298}{0.250} = \frac{110.3}{0.250} = 44.1\ \text{g mol}^{-1}

This gives CO2\text{CO}_2 (M=44.01 g mol1M = 44.01\ \text{g mol}^{-1}), which is correct.

Origin question: Yes, the line should be forced through the origin because when P=0P = 0, there is no gas in the container, so mm must equal 00. The relationship m=(MV/RT)Pm = (MV/RT)P has no intercept term. However, in practice, a best-fit line not forced through the origin may reveal systematic error (e.g., the container was not fully evacuated).

Integration Tests

IT-1: Error Analysis in a Titration (with Acids and Bases)

Question: In a titration of HCl\text{HCl} with NaOH\text{NaOH}, a student uses a burette (±0.05 cm3\pm 0.05\ \text{cm}^3) and a pipette (±0.05 cm3\pm 0.05\ \text{cm}^3). The pipette delivers 25.00 cm325.00\ \text{cm}^3 of 0.100±0.001 mol dm30.100 \pm 0.001\ \text{mol dm}^{-3} HCl. The average titre is 24.85 cm324.85\ \text{cm}^3. Calculate the concentration of NaOH with its absolute uncertainty. The titre range is 24.8024.80--24.90 cm324.90\ \text{cm}^3.

Solution:

n(HCl)=c×V=0.100×25.00/1000=2.500×103 moln(\text{HCl}) = c \times V = 0.100 \times 25.00/1000 = 2.500 \times 10^{-3}\ \text{mol}

n(NaOH)=n(HCl)=2.500×103 moln(\text{NaOH}) = n(\text{HCl}) = 2.500 \times 10^{-3}\ \text{mol} (1:1 stoichiometry)

c(NaOH)=2.500×10324.85/1000=2.500×1030.02485=0.1006 mol dm3c(\text{NaOH}) = \frac{2.500 \times 10^{-3}}{24.85/1000} = \frac{2.500 \times 10^{-3}}{0.02485} = 0.1006\ \text{mol dm}^{-3}

Uncertainty analysis:

Fractional uncertainty in c(HCl)c(\text{HCl}): 0.001/0.100=0.0100.001/0.100 = 0.010 (1.0%)

Fractional uncertainty in V(HCl)V(\text{HCl}): 0.05/25.00=0.00200.05/25.00 = 0.0020 (0.20%)

Fractional uncertainty in V(NaOH)V(\text{NaOH}): The range 24.8024.80--24.9024.90 gives a spread of 0.10 cm30.10\ \text{cm}^3. Half-range =0.05 cm3= 0.05\ \text{cm}^3. Fractional: 0.05/24.85=0.00200.05/24.85 = 0.0020 (0.20%).

Total fractional uncertainty in c(NaOH)c(\text{NaOH}): 0.0102+0.00202+0.00202=0.0001+0.000004+0.000004=0.000108=0.0104\sqrt{0.010^2 + 0.0020^2 + 0.0020^2} = \sqrt{0.0001 + 0.000004 + 0.000004} = \sqrt{0.000108} = 0.0104 (1.04%).

Absolute uncertainty: 0.1006×0.0104=0.00105 mol dm30.1006 \times 0.0104 = 0.00105\ \text{mol dm}^{-3}.

c(NaOH)=0.101±0.001 mol dm3c(\text{NaOH}) = 0.101 \pm 0.001\ \text{mol dm}^{-3}

The concentration uncertainty is dominated by the uncertainty in the HCl concentration.


IT-2: Propagation of Uncertainty in Kinetics (with Kinetics)

Question: The Arrhenius equation lnk=lnAEa/RT\ln k = \ln A - E_a/RT is used to determine EaE_a from a plot of lnk\ln k vs 1/T1/T. A student obtains a gradient of 8500 K-8500\ \text{K} with a standard error of ±200 K\pm 200\ \text{K}. Calculate EaE_a and its uncertainty. If the y-intercept is 25.0±0.525.0 \pm 0.5, calculate AA and its uncertainty.

Solution:

Gradient=Ea/R\text{Gradient} = -E_a/R, so Ea=gradient×RE_a = -\text{gradient} \times R.

Ea=8500×8.314=70669 J mol1=70.7 kJ mol1E_a = 8500 \times 8.314 = 70669\ \text{J mol}^{-1} = 70.7\ \text{kJ mol}^{-1}

Uncertainty: ΔEa=200×8.314=1663 J mol1=1.7 kJ mol1\Delta E_a = 200 \times 8.314 = 1663\ \text{J mol}^{-1} = 1.7\ \text{kJ mol}^{-1}

Ea=70.7±1.7 kJ mol1E_a = 70.7 \pm 1.7\ \text{kJ mol}^{-1}

For the pre-exponential factor: lnA=intercept=25.0\ln A = \text{intercept} = 25.0.

A=e25.0=7.20×1010A = e^{25.0} = 7.20 \times 10^{10} (with units depending on the reaction order)

Uncertainty in AA: The intercept uncertainty is ±0.5\pm 0.5. Since A=einterceptA = e^{\text{intercept}}:

Amax=e25.5=1.18×1011A_{\max} = e^{25.5} = 1.18 \times 10^{11}, Amin=e24.5=4.39×1010A_{\min} = e^{24.5} = 4.39 \times 10^{10}

ΔA=1.18×10114.39×10102=3.71×1010\Delta A = \frac{1.18 \times 10^{11} - 4.39 \times 10^{10}}{2} = 3.71 \times 10^{10}

A=(7.2±3.7)×1010 dm3mol1s1A = (7.2 \pm 3.7) \times 10^{10}\ \text{dm}^{3}\text{mol}^{-1}\text{s}^{-1} (for a second-order reaction)

The large relative uncertainty in AA (about 51%) reflects the exponential sensitivity: a small uncertainty in the intercept produces a large uncertainty in AA. This is why EaE_a is generally determined more precisely than AA from Arrhenius plots.


IT-3: Statistical Analysis and Equilibrium (with Equilibrium)

Question: A student measures KcK_c for the reaction N2O42NO2\text{N}_2\text{O}_4 \rightleftharpoons 2\text{NO}_2 five times and obtains: 4.2×1034.2 \times 10^{-3}, 4.8×1034.8 \times 10^{-3}, 4.5×1034.5 \times 10^{-3}, 4.1×1034.1 \times 10^{-3}, 4.6×1034.6 \times 10^{-3}. Calculate the mean, standard deviation, and 95% confidence interval. The literature value is 4.6×1034.6 \times 10^{-3}. Does the experimental value agree with the literature value?

Solution:

Mean: xˉ=4.2+4.8+4.5+4.1+4.65×103=22.25×103=4.44×103\bar{x} = \frac{4.2 + 4.8 + 4.5 + 4.1 + 4.6}{5} \times 10^{-3} = \frac{22.2}{5} \times 10^{-3} = 4.44 \times 10^{-3}

Standard deviation:

Deviations: 0.24,+0.36,+0.06,0.34,+0.16-0.24, +0.36, +0.06, -0.34, +0.16 (all ×103\times 10^{-3})

s=(0.24)2+(0.36)2+(0.06)2+(0.34)2+(0.16)251×103s = \sqrt{\frac{(-0.24)^2 + (0.36)^2 + (0.06)^2 + (-0.34)^2 + (0.16)^2}{5 - 1}} \times 10^{-3}

s=0.0576+0.1296+0.0036+0.1156+0.02564×103=0.33204×103=0.0830×103=0.288×103s = \sqrt{\frac{0.0576 + 0.1296 + 0.0036 + 0.1156 + 0.0256}{4}} \times 10^{-3} = \sqrt{\frac{0.3320}{4}} \times 10^{-3} = \sqrt{0.0830} \times 10^{-3} = 0.288 \times 10^{-3}

Standard error of the mean: SEM=sn=0.288×1035=0.129×103\text{SEM} = \frac{s}{\sqrt{n}} = \frac{0.288 \times 10^{-3}}{\sqrt{5}} = 0.129 \times 10^{-3}

95% confidence interval (using t0.025,4=2.776t_{0.025, 4} = 2.776):

CI=xˉ±t×SEM=(4.44±2.776×0.129)×103=(4.44±0.36)×103\text{CI} = \bar{x} \pm t \times \text{SEM} = (4.44 \pm 2.776 \times 0.129) \times 10^{-3} = (4.44 \pm 0.36) \times 10^{-3}

Range: (4.08 to 4.80)×103(4.08 \text{ to } 4.80) \times 10^{-3}.

The literature value 4.6×1034.6 \times 10^{-3} falls within the 95% confidence interval, so the experimental result agrees with the literature value at the 95% confidence level.