Spectrophotometry Practical

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Introduction[✎ edit | edit source]

Spectroscopy is the study of origin and aspects of the entire electromagnetic spectrum as well as interactions between matter and electromagnetic radiation. It examines relations of absorption, emission or dispersion of electromagnetic radiation as a function of wave length (λ) or frequency (f). If certain tests are carried out, it is possible to gain information about quantity and quality of the examined substance. Spectrophotometry is a subcategory of spectroscopy as it studies only the quantity of spectrums. This includes the amount of reflected and absorbed light as well as of the light that passes through substance in relation to waveleght.

One of the characteristic optical properties of substances is absorption of electromagnetic radiation. During an interaction of certain wavelength of light with substance molecules, energy of photon is used for excitation of valence electrons. Intensity of light that passes through (I) is therefore lower than intensity of incident beam (lo). Lambert’s law applies here.

[math]I=I_0 \cdot 10^{-\mu \cdot l}[/math]

l is a thickness of absorbing layer and µ is called linear absorption coefficient. Ratio of passed through and incidental light is known as transmittance (T).

[math]T=\frac{I}{I_0}[/math]

It reaches values ranging from 0 (all light was absorbed) to 1 (all light passed through; if fluorescent substances are being used, it can reach values higher than 1). Negative decadic logarithm of transmittance is absorbance (A). Following then applies:

[math]A=-log T = -log \left ( \frac{I}{I_0} \right ) = \mu\cdot l[/math]

Spectrum created by light passing through a substance is called spectrum of absorption and is dependent on absorbance or on wave length.

For absorption in solution, Beer's law says: absorption coefficient of a solution is linearly proportional to concentration. Concentration (c) is molar in most cases and thus ε (constant of proportionality) is called molar absorption coefficient ε. It is specific for every individual substance and wave length. When combined, these two relations form Lambert-beer’s law. [math]A=\varepsilon\cdot l\cdot c[/math](With this knowledge, it is possible to use this relation for transmittance: [math]T = 10^{-\epsilon \cdot l \cdot c}\,\![/math])

Absorbance is linearly proportional to concentration (c) of substance and to thickness of absorbing layer (l), which is the length of optical path or width of cuvette (usually 1 cm). Lambert-beer’s law applies only if monochromatic light is used, length of cuvette is constant, same solvent is used (influence of pH, temperature) and when analectic concentration of the substance is in its absorbing form.

Spectroscopic properties in visible (VIS) and ultraviolet (UV) are studied in spectroscopy and photometry. They use light the UV area (wavelength 10-390 nm), visible areas (wavelength 390-790 nm) and adjacent infrared areas (wavelength 770 nm - 1 mm). Thanks to the Lambert-beer’s law, it is possible to determine concentration of unknown solutions. This can be done using two different methods: calibration curve method (see task 2) and standard addition method.

Calibration curve method - Absorbance of several calibration samples is measured. All samples have different concentrations but are placed in the same cuvettes and the same wave length is used to measure them. From the course of the calibration curve, Lambert-beer’s law can be verified. The resulting dependence should be in ideal case linear. so called calibration curve.  However, this method is only viable for simple matrix such as fresh water.

Standard addition method - Absorbance of unknown sample (Avz) is measured. Thereafter the concentration of the substance in the sample is increased by the defined standard addition and corresponding absorbance of the solution is measured. This method is used in complex matrix such as wastewater, where application of calibration curve method would be quite difficult.

Determining concentration of unknown substance via linear regression

Let’s express the theoretical dependency of measured absorbance of a sample on concentration via equation of linear regression y = a + b · x. The formula of the linear regression equation is based on the Lambert-Beer law. It contains two variables (x, y) and two regression coefficients (a, b). Both variables can be easily replaced with the magnitude from the graph of the calibration curve which expresses the concentration of the absorbance on the concentration which means that x means concentration (c) and y absorbance (A). The correct equation should be A = a + b · c.

Regression coefficient a expresses possible systematic error of measurement (or deviations caused by dirt on cuvette or similar). We “filter” these errors out by its assumptions.

Linear term b · c represents “clean” Lamber-Beer law. According to it, absorbance of solution is A = ε · l · c. Concentration is in both expressions thus, we can say that coefficient of regression b is equal to multiplication of molar extinct coefficient and width of cuvette: b = ε · l. This element expresses slope of a line in regression equation. From here we determine molar extinction coefficient ε = b / l. But we must pay attention on units because concentration is in micromole per liter (μMol/L), while width of cuvette is in centimeters.

Measuring Principle[✎ edit | edit source]

Photometers and spectrophotometers are used for spectrophotometric assays. Devices which measure in one or more specifically defined wavelengths of monochromatic lights are called photometers. More technically advanced devices where you can set or measure any wavelength of monochromatic light are called spectrophotometers. They measure intensity of light after going through sample (I) and put it in ratio with intensity of light before going through sample (I0). Based on mentioned relations it is possible to determine transmittance, absorbance, and sample concentration.

Spectrophotometer is made of these parts

• Light source (halogen light for visible light, deuterium for UV area)

• Lenses and mirrors that direct the beam of light

• Monochromator (device transmitting light of a certain wavelength) – Nowadays optical grids are usually used. which allow the wavelength to change fluently. The range of wavelengths depends on the slot – it can be changed or permanently preset from the factory. The wider the slot is the more intense the resulting light coming out of the machine but this causes less specific measurements.

• Cuvette space – Space for samples in cuvettes from plastic, glass or quartz glass

• Detector (Charge-coupled device or photodiode) – Accuracy depends on integration time – time at which the absorbance is measured. Increased time results in increased accuracy of the measurement, except for photosensitive substances (i.e. the substance won’t fade out at longer exposure of light). Disadvantages of longer integration time are also longer measurement times, which is very important when processing a larger number of samples, when using larger number of wavelengths (i.e. measuring more spectrums), or when processing samples which are changing over time (kinetic measurements)

• Output device (software for data analysis)

Based on the number of beams used for measuring, we distinguish single or double-beam spectrophotometers. Double-beam spectrophotometers use one beam for measuring the sample, and the other for blank (solvent without the substance). When using the single-beam device we must first measure attributes of blank and then measure the sample.

Modern spectrophotometers are fully automatized and controllable via computers. They are used for measuring absorbing specters (wider spectrum of wavelengths) or quantitative measurement (for one or more wavelengths). They can also be used for measuring kinetics of simple, for example enzymatic reactions. Thus, it’s used in a wide range of scientific disciplines such as chemistry, physics, biochemistry, biology and even medicine.

In practice the validity of Lamber-Beer law is limited by dispersion of light because of tiny impurities in the sample; phosphorescence or fluorescence of the sample; small amount of light passing through highly concentrated solutions; changes of values of absorbing coefficients; shifting chemical equilibrium caused by high concentration of substances in the sample.

Importance in clinical medicine[✎ edit | edit source]

Spectrophotometer being used in a hospital

Spectrophotometers are of high clinical importance in almost all branches of medicine.

Their ability to measure concentrations of metabolically important substances in body fluids, such as blood, cerebrospinal fluid, urine and amniotic fluid among others, is crucial for correct diagnostic findings and continuous monitoring of patients.  Equally early identified small deficiencies of certain essential substances might help preventing correlated health problems.

In intensive medicine the use of spectrophotometric analyses is more frequent, due to the fact that patients in unstable states are more prone to drastic changes in the amount of different substances in, for example, their blood. Intensive care units therefore frequently have spectrophotometers on site whereas general practitioners might send their probes to be analyzed in a laboratory.

The substances that can be quantitatively analyzed by spectrophotometers are numerous. They include: hemoglobin, erythrocytes, hematocrit, amylase, bilirubin, cholesterol, glucose, urea, creatinine, lipase, triglyceride, albumin, alcohol, ammonia, copper, magnesium, lactate, calcium, iron, magnesium, aluminium, sodium carbonate, carbon monoxide and even certain enzymes.

BRIEF literature review[✎ edit | edit source]

What are its advantages and disadvantages?[✎ edit | edit source]

Spectrophotometer are very complex instruments that use different monochromatic lights in purpose to give an information to the researcher. Most of the times in medicine, the information sought is a concentration of one or multiple compounds. These compounds have a specific absorbance spectrum corresponding to their molecular structure. In most cases, researchers use calibration methods with known concentrations of the researched compound, plot a best fit curve and are then able to be find other concentrations from the curve (Musiol). Each measurement is to be done in the same environment which enables a very small risk of error.

An inconvenience of using spectrophotometry is that measurements have to be taken meticulously. Any trace of fingertips or condensation on the cuvettes can create random error in measurements, and therefore the use of microfiber paper is recommended (Musiol). Microfiber has for effect to clean any potential dust on the transparent side of the cuvettes. It also has no risk to create small abrasions on the cuvette. Another limitation to the precision of spectrophotometers can be the precision of the tools used to make the calibration concentrations such as pipettes, also source to random error.

How does it work?[✎ edit | edit source]

Schematic Diagram of a Spectrophotometer

A spectrophotometer consists of 6 basic components. A light source is needed, generally a deuterium lamp and a Halogen lamp are used. The use of two different sources of light provides the analysis device with wider wavelength of light and therefore a more versatile use. Then the light can either go through a monochromator containing diffraction grating or not, depending on the nature of the measurement. A monochromator will enable only a certain wavelength (in nm) to go through the aperture.

In case no monochromator is used, a light containing all visible wavelengths is emitted and goes through the sample. The light then exits the sample, enters a closed compartment through the exit slit and hits the charged coupled device (CCD). The CCD will have a certain number of light sensors that will react with the photons of the light given. The information given by the CCD will then be transferred to a computer software which will be able to read and display the transmittance of a compound at MULTIPLE wavelengths. The CCD needs to be calibrated posteriorly to the measurements with a reference cuvette of distilled water for example. This reference cuvette will indicate to the software the amount of LIGHT ABSORBED BY THE SOLVENT AND CUVETTE MATERIALS ONLY and at all the wavelengths of the visible light.

Are there any risks involved in it’s use (for patients and the clinical staff)?[✎ edit | edit source]

The use of spectrophotometers is safe. The deuterium lamp represents no danger as it is filled with Hydrogen gas. Even if certain Spectrophotometers use UV light, it is enclosed and therefore cannot unwillingly harm us.

Are there ethical issues associated with the topic?[✎ edit | edit source]

There is no real ethical issues associated with spectrophotometry.

The equipment[✎ edit | edit source]

Spectrophotometer
  1. Spectrophotometer
  2. Cuvette
  3. Blank solution
  4. Computer
  5. Unknown solution

The methodology[✎ edit | edit source]

The SPECORD 40 spectrophotometer is a single-ray spectrophotometer operating in the wavelength range from 190 to 1100 nm (using a deuterium lamp for the 190–300 nm range and a halogen lamp for the 300–1100 nm range). It is used for measuring absorbance values in the interval of A values from –3 to +3. It can be controlled from the main panel or using the WinAspect program which simultaneously permits a simple and rapid data analysis. Safety advice For work with solutions of malachite green and indigotin wear protective gloves. Do not inhale or consume the solution. The spectrophotometer is sensitive to humidity. Be careful when working with liquids. After accidental spilling dry the affected area immediately.


Task 1. Measurement of absorption spectrum Measurement, define and characterize the absorption spectrum of a solution of malachite green and indigotin.

Chemicals: • Solutions A and B • Distilled water

Working procedure

1. Turn on the spectrophotometer and the PC

2. Turn on the WinAspect program.

3. Open the Measurement menu and select Initialize device. After confirmation, the question appears on the use of a UV lamp which is to be rejected. The spectrophotometer then runs automatically initialization and internal calibration.

4. After termination of initialization set the measurement parameters. In the Measurements menu select Set parameters. A panel for setting the parameters will appear and you should click on New. Setting the parameters

The Settings panel: In the Title window fill in the name. Function Cycle Mode deactivated by selecting the possibility None Function Display – select the possibility Absorbance Function Correction – select the possibility Reference

The Mode panel: In the Meas.Mode window select the possibility Scan Mode Setting the Scan Mode function with the following values: Range = 375–675 nm (width of the examined spectrum) Delta lambda = 1 nm (length of the measurement intervals) Speed = 50 nm/s (speed of measurement)

After setting the parameters click on the green check sign OK as on the measurement setting panel. The window with possibilities of saving will appear and you save the file in the Para folder under the name ENXXX SCAN. After saving click on OK icon.

5. The spectrophotometer is now ready for the measurement itself. The Measurement panel opens and you select Serial measurement.

6. In the WinASPECT program a window for Serial Measurements is now open. To set the parameters of measurement select from the Edit dialog box in the instrument panel the possibility Setup.

Set the following parameters: Panel General: Description: enter ENXXX SCAN Panel Samples: Number of measurements: enter the number of samples (2 in this case).


7. Before sample measurement, it is essential to carry out a reference measurement of the blank (solvent without dissolved substance). The samples are substances dissolved in distilled water hence the blank should be distilled water in a cuvette filled to about two-thirds height.

The cuvette should be held at the mat side. The light ray passes through the clear sides and their contamination (including fingerprints) can result in affecting the measurement results. Dry the cuvette before measurement and remove any impurities and fingerprints with dry cotton wool.

Cuvette

8. Open the sample compartment. The cuvette with the blank should be placed into the holder. Close the door of the sample compartment.

The cuvette should be placed as close as possible to the holder wall to permit full transmittance of the light beam through the clear walls. Make sure that the cuvette is placed vertically in the holder.

The spectrophotometer can be damaged by spilled liquids. Be careful when working with it and, if a spill occurs, dry the affected place carefully.

9. Start the reference measurement by clicking on Reference in the instrument panel of the Serial Measurement window. The spectrophotometer registers the absorption spectrum of the blank.


10. After the reference measurement the spectrophotometer is ready for sample measurement. This is started by clicking on the Start icon. Pour the first sample into a clean cuvette and place it in the holder (see points 8 and 9). Close the sample compartment (spectrophotometer lid) and confirm the action in the program (OK). The spectrophotometer will measure the absorption spectrum of the first sample.


11. After the first sample measurement repeat the procedure with the second sample. During sample measurement try to proceed from the most dilute to the most concentrated sample. Then you need not to rinse the cuvette after each measurement.

12. After termination of all measurements, a table containing the measured values of absorbance at the given wavelength (Table panel) or a graphical representation of the tabulated values (Graphic panel) will appear.

13. By clicking on an icon To document you will transform results into document form. Save it using your group name.

14. Print the page containing results

Task 2. Determination of concentration of an unknown sample and the Lambert-Beer law On the basis of absorbances of samples of known concentration construct calibration curve. Determinate concentration of an unknown sample on the basis of the Lambert-Beer law.

Working procedure

Calibration curve

Before starting the assignment use the spectra obtained in Task no. 1 to determine a suitable wavelength for measuring the absorbance of solutions A and B and for both solutions in mixture (answer to questions asked in Task no. 1 report)

Since you are working with two substances a calibration curve must be constructed for both of them separately. Calibration curve for samples KA 1–4

1. In the WinASPECT program choose Quant on the instrument panel and the possibility Calibration.


2. The monitor will display the Calibration window for setting measurement parameters.

Screen General Designation group: ENXXXQUANTKA Regression Model: choose possibility y = A + B*x WAVELENGTH1 (most suitable for solutions A and B): choose on the basis of values obtained in Task 1. Calibration units should be chosen according to units used for calibration samples characterization (see table of concentrations). Ordinate: absorbance Cell Pathlength: measure the width of the cuvette Number of Standards: 4 for KA


3. Click on Edit icon, choose Measurement parameters. On the Mode panel choose from the offer Meas. mode the possibility Wavelengths. The suitable wavelength is selected by clicking on Edit. By clicking on Edit icon you choose the suitable wavelength and by clicking on OK and subsequent choice confirmation you return to the Calibration offer.


4. After returning to Calibration and entering the above parameters click on Standards icon.

5. Now the window will open; enter the individual standards in corresponding units. Start with the lowest concentration KA1.

Standard: enter the names of standards Conc.: enter the concentration values Source: this value is entered automatically


6. Don't click on the green check sign OK - it cause the measurement termination.

7. Measure the absorbance of the blank. A cuvette with distilled water should be placed in the holder and by clicking on Reference carry out the reference measurement.

8. Click on Start and place the KA1 sample in the holder. Then measure KA1, KA2, KA3 and KA4 in this sequence. After termination of measurement click on OK.

9. The Calibration window now opens, containing a graphical representation of the calibration curve and the regression line equation.

10. After clicking on To conc. (measurement of samples of unknown concentration) the calibration curve can be saved. After a positive answer (dialogue window) save the file under XXXKALIBKA in the Calib file.

Determination of concentration of an unknown sample (for sample NA)

11. After saving the program will automatically open the Concentration window which enables to determine the concentration of unknown samples from a calibration curve.

12. To measure the concentrations of unknown samples place the sample in a cuvette into the clamp and by clicking on Start (Meas.) the instrument will measure the absorbance and, on the basis of calibration curve coefficients, will calculate the concentration of the unknown sample.

13. On the same principle we obtain the concentrations of NA1, NA2. NA3 and NA4.

14. After termination of the measurement the concentration values will appear in a table.

15. Save the document as ENXXXQUANTNA.

16. After measurement clean used cuvettes.

Conclusion[✎ edit | edit source]

The future of spectrophotometry lies especially in the improvement of pathological diagnostics, disease detection and general clinical research as “uv-vis spectroscopy enables safer, non-invasive analysis of soft tissue, and can enhance accuracy and speed in clinical diagnostics and medical research.”

Around 10% of cancers are due to the exposure of radiation, therefore, such improvements will aid us in the advancement of clinical applications relating to various types of cancers. Spectrophotometry has enabled us to “convert measured reflectance and fluorescence spectra from tissue to cancer-relevant parameters such as vascular volume, oxygenation, extracellular matrix extent, metabolic redox states, and cellular proliferation.” Pulse oximetry is a method of examining a person’s oxygen saturation and it uses the means of in vivo spectrophotometry in its procedure. This relatively recent method of examination also presents several possibilities for future developments of spectrophotometry by providing “reliable, objective, and non-invasive” results.

Bibliography[✎ edit | edit source]

Musiol, Tanja, Dr. "Troubleshooting in UV/Vis Spectrophotometry." Biocompare. Biocompare, 18 Feb. 2013. Web. 11 Dec. 2016.

How Does a Spectrometer Work?" B&W Tek. B&W Tek, 2016. Web. 12 Dec. 2016.

Anand, Preetha, Ajaikumar B. Kunnumakara, Chitra Sundaram, Kuzhuvelil B. Harikumar, Sheeja T. Tharakan, Oiki S. Lai, Bokyung Sung, and Bharat B. Aggarwal. "Cancer Is a Preventable Disease That Requires Major Lifestyle Changes." Pharmaceutical Research. Springer US, Sept. 2008. Web. 19 Dec. 2016

[https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2742920/>. Brown, J. Quincy, Karthik Vishwanath, Gregory M. Palmer, and Nirmala Ramanujam. "Advances in Quantitative UV-Visible Spectroscopy for Clinical and Pre-clinical Application in Cancer." Current Opinion in Biotechnology. U.S. National Library of Medicine, Feb. 2009. Web. 19 Dec. 2016.]

COFFEY, VALERIE C. "Trends in Spectroscopy: IR, UV-VIS Techniques Are Safe, Speedy and Skin-Deep." N.p., Dec. 2013. Web. 19 Dec. 2016.

Wagner, JL, and Ruskin, KJ. "Pulse Oximetry: Basic Principles and Applications in Aerospace Medicine." Aviation, Space, and Environmental Medicine. U.S. National Library of Medicine, Oct. 2007. Web. 25 Dec. 2016.

“Manuelle Photometer.” n.d. Web. 25 Dec. 2016.

Applications of absorption spectroscopy (UV, visible). 2008. Web. 25 Dec. 2016.

Lewen, N. “The Use of Atomic Spectroscopy in the Pharmaceutical Industry for the Determination of Trace Elements in Pharmaceuticals.” Journal of pharmaceutical and biomedical analysis. 55.4 (2010): 653–61. Web. 25 Dec. 2016.

Decker, Walter J. “Atomic Absorption Spectroscopy: Applications in Agriculture, Biology, and Medicine.” Archives of Internal Medicine 128.4 (1971): 649–650. Web. 25 Dec. 2016.

2015. Fabulously versatile uses of a spectrophotometer. Buzzle, 29 Sept. 2016. Web. 25 Dec. 2016.

Levere, R D, F Swerdlow, and M R Garavoy. “Measurement of Human Plasma Hemoglobin by Difference Spectrophotometry.” 77.1 (1971): 168–76. Web. 25 Dec. 2016.

Translation of wikiskripta:Spektrofotometrie pro praktická cvičení 2.LF UK (3 Dec. 2018)