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Beer's Law & Spectrophotometry Lab

Choose a colored solution, set the molar absorptivity and cuvette path length, then build a calibration curve from known concentrations. The lab computes absorbance and percent transmittance for each standard, fits a linear trendline, and back-calculates the concentration of an unknown sample from a measured absorbance.

Guided Experiment: Beer's Law Standard Curve

If you prepare solutions of KMnO₄ at concentrations from 0.0002 to 0.001 M, how do you predict absorbance will change as concentration increases? Will the relationship be linear?

Write your hypothesis in the Lab Report panel, then click Next.

Cuvette View
LightsourceDetector%T = 3.6path length bA = 1.440
Standard CurveR² = 1.0000
Concentration (M)Absorbance0.000.601.201.802.4000.25m0.50m0.75m0.0010Unknown

Controls

λmax = 525 nm. Intense purple; common in titrations and water treatment

M⁻¹cm⁻¹
cm
Standard Concentrations
M
M
M
M
M

Results

Standard Curve Fit
Slope (expected ε·b)2400.00 M⁻¹
Expected ε·b2400.00 M⁻¹
Intercept-0.0000
1.0000
Standard Points
c (M)A%T
2.00e-40.480033.11
4.00e-40.960010.96
6.00e-41.44003.63
8.00e-41.92001.20
1.00e-32.40000.40
Unknown Sample
Measured Absorbance0.4800
Percent Transmittance33.11 %
Calculated Concentration2.0000e-4 M

Data Table

(0 rows)
#TrialConcentration (M)Absorbance (A)%T
0 / 500
0 / 500
0 / 500

Reference Guide

The Beer-Lambert Law

The Beer-Lambert Law relates the attenuation of light to the properties of the material it passes through. For a solution in a cuvette:

A=εbcA = \varepsilon \cdot b \cdot c

where A is absorbance (dimensionless), ε (epsilon) is the molar absorptivity in M⁻¹cm⁻¹, b is the path length in cm, and c is the concentration in mol/L. Absorbance is directly proportional to concentration when ε and b are held constant.

Absorbance and Transmittance

Transmittance T is the fraction of incident light that passes through the sample. Percent transmittance %T = 100 T. Absorbance and transmittance are related by a base-10 logarithm:

A=log10(T)=log10 ⁣(II0)A = -\log_{10}(T) = -\log_{10}\!\left(\frac{I}{I_0}\right)

An absorbance of 1 corresponds to 10% transmittance. An absorbance of 2 means only 1% of light passes through. At A = 0 the solution is perfectly transparent (%T = 100).

Standard Curve and Calibration

A standard curve (calibration curve) is constructed by measuring the absorbance of several solutions of known concentration. Plotting A on the y-axis against c on the x-axis gives a straight line through the origin with slope equal to ε · b.

To find the concentration of an unknown sample, measure its absorbance and read the corresponding concentration from the standard curve, or use:

cunknown=Aunknownεbc_{\text{unknown}} = \frac{A_{\text{unknown}}}{\varepsilon \cdot b}

Molar Absorptivity and Wavelength

The molar absorptivity ε is a molecular constant that describes how strongly a chemical species absorbs light at a given wavelength. It depends on the electronic structure of the molecule. Solutions should be measured at their wavelength of maximum absorbance (λmax) to maximise sensitivity.

KMnO₄ at 525 nm has ε ≈ 2400 M⁻¹cm⁻¹. FD&C Blue 1 at 630 nm has ε ≈ 130,000 M⁻¹cm⁻¹, so far lower concentrations are needed for the same absorbance reading.

Real-World Applications

Spectrophotometry is used across science and industry. In clinical labs, blood glucose, hemoglobin, and bilirubin are measured photometrically. Environmental chemists use Beer's Law to quantify nitrate, phosphate, and heavy metal contamination in water.

In biochemistry, protein concentrations are measured by the Bradford or BCA assay, and DNA/RNA purity is assessed at 260 nm and 280 nm. Industrial quality control uses spectrophotometry to verify dye concentrations in textiles, beverages, and pharmaceuticals.

Deviations from Beer's Law

Beer's Law assumes ideal conditions that break down at high concentrations. Above roughly 0.01 M, solute molecules begin to interact with each other, changing their effective absorptivity. The relationship between A and c curves downward, so the standard curve is no longer linear and the method becomes unreliable.

Instrumental deviations include stray light reaching the detector and non-monochromatic radiation. Stray light causes the absorbance to plateau at high concentrations, a common source of error in student experiments. Always work within the linear range of your standard curve (typically A between 0.1 and 1.5).

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