Why do proteins absorb uv light




















Tyrosine can be excited at wavelengths similar to that of tryptophan but will emit at a distinctly different wavelength. While it may be true that tyrosine is less fluorescent than tryptophan, it can provide significant signal since it is often present in large numbers in many proteins.

Tyrosine fluorescence has been observed to be quenched by the presence of nearby tryptophan moieties either through resonance energy transfer or the ionization of its aromatic hydroxyl group.

Here are some important points to remember when measuring peptides using the A method. This assay is suitable for the simple and rapid estimation of protein concentration. This assay is based on a single Coomassie dye based reagent. The binding of protein to the dye results in a change of color from brown to blue.

The change in color density is proportional to protein concentration. Protein estimation can be performed using as little as 0. As such, protein fluorescence requires very powerful UV light sources and very sensitive cameras because the fluorescent emission from proteins is so weak. However, powerful UV light sources can destroy the protein due to long exposure times required to obtain significant data.

A much faster way to image proteins, either in cells, tissues or as crystals, is to utilize their strong absorption of UV light as a contrasting mechanism. By using a ultraviolet microscope or microspectrophotometer equipped for UV imaging, the sample containing the protein is imaged with nm light.

The protein will absorb this light more strongly than the surrounding sample and will appear darker. See the picture above for an example of UV absorption of a protein crystal in salt solution. This technique is very fast, exposing the protein to UV light for far less time.

CRAIC Technologies microspectrophotometers are used to acquire spectra of microscopic samples containing proteins, such as individual protein crystals, by their UV absorption. The microspectrophotometer consists of a UV-visible-NIR range microscope integrated with a spectrophotometer. As such, it is able to measure the UV-visible-NIR spectra of microscopic samples of tissue, protein crystals and other protein containing structures. By using absorption, it is able to measure these samples quickly and non-destructively.

Microspectroscopy allows the user to learn more about the optical features and the chemical structure of the protein. Note that BSA protein, which has an absorbance value at nm similar to that of tryptophan, has less absorbance at nm as a result of fewer aromatic rings on a molar basis. Figure 2. Absorbance Spectral scans of aromatic amino acids and bovine serum albumin BSA.

Spectral scans from nm to nm in 1 nm increments were performed on the amino acids, tryptophan, tyrosine and phenylalanine, as well as BSA protein in aqueous solution using a Synergy HT multi-detection microplate reader. Using the monochromator to select excitation wavelength, precise tuning of the excitation wavelength is possible. Interestingly enough, the background fluorescence of the microplate was observed to vary quite dramatically over the same excitation wavelengths. Therefore it is important to examine the corrected signal i.

Using the data from Figure 3, an excitation wavelength of nm was used for subsequent determinations of L-tryptophan. Figure 3. Excitation peak determination for L-tryptophan in solution. All readings were obtained using the same sensitivity setting of and the blank value at that wavelength subtracted. Using the optimized excitation wavelength, several dilutions of L-tryptophan were aliquoted into a microplate and the fluorescence measured.

The resultant concentration curve plotted in KC4 software demonstrates a linear relationship between L-tryptophan concentration and fluorescence Figure 4. Concentration determinations can be made with a high degree of confidence, as the correlation coefficient r2 for the linear regression analysis was calculated to be 0. Using fluorescence, the limit of detection of L-tryptophan was found to be Figure 4.

Tryptophan Concentration Curve. A series of dilutions of L-tryptophan were made using distilled water as the diluent. Readings were made from the top using a sensitivity setting of The peak excitation wavelength for L-tyrosine was determined in a similar fashion as described for tryptophan.

Figure 5 demonstrates that wavelengths between nm and nm produce equivalent blank-subtracted fluorescent signals. Subsequent experiments used nm as the excitation wavelength. Several dilutions of L-tyrosine were then aliquoted into a microplate and the fluorescence measured. Using a least means squared linear regression analysis, the correlation coefficient r2 was greater than 0.

Figure 5. Excitation peak determination for L-Tyrosine in solution. All readings were obtained using the same sensitivity setting of and the value of the blank at that wavelength subtracted. Figure 6. Tyrosine Concentration Curve. Several dilutions of L-tyrosine were prepared using deionized water as the diluent. The lone pairs on a carbonyl group can absorb at higher wavelengths than benzene. These involve electronic transitions between a non-bonding electron to the LUMO; the transition energy is so low because a non-bonding electron does not have its energy lowered like a bonding orbital.

The gap between a non-bonding orbital and anti-bonding orbital is therefore much smaller than usual. There was a good post on pi-conjugation elsewhere on the site, here. You can read more about carbonyl excitations here. For general excitation values, this page was useful.

As far as the molecule is concerned there is no distinction between visible and uv light. In each case the transition is from a ground state to an electronically excited state. This is caused by a photon being absorbed and its energy taken up by the molecule. In doing so an electron is promoted from a lower orbital to a higher one.

The conjugation in a molecule lowers the orbital energy because, in effect, an electron is able to 'spread out' and is not confined to be associated with just two atoms.

Thus the greater the extent of conjugation the lower the orbital energy and the smaller the energy gap between the ground state and lowest excited state. You can think of this rather like a particle in a box, the longer the box the lower and closer the energy of the various levels becomes. In addition to the lowest electronic transitions there are transitions to higher electronic states, where an electron is promoted to a higher anti-bonding orbital than the LUMO.

Each electronic state so produced also has its own set of rotational and vibrational levels in the same way to the the ground state. Thus the spectrum can become congested even when molecules are studied in the low pressure vapour phase where the influence of collisions with other molecules and solvent is absent. Sign up to join this community.



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