Copper proteins are proteins that contain one or more copper ions as prosthetic groups. Copper proteins are found in all forms of air-breathing life. These proteins are usually associated with electron-transfer with or without the involvement of oxygen (O2). Some organisms even use copper proteins to carry oxygen instead of iron proteins. A prominent copper protein in humans is in cytochrome c oxidase (cco). This enzyme cco mediates the controlled combustion that produces ATP.[1] Other copper proteins include some superoxide dismutases used in defense against free radicals, peptidyl-α-monooxygenase for the production of hormones, and tyrosinase, which affects skin pigmentation.[2]
The metal centers in the copper proteins can be classified into several types:[3]
The blue copper proteins owe their name to their intense blue coloration (Cu(II)). The blue copper protein often called as “moonlighting protein”, which means a protein can perform more than one function. They serve as electron transfer agents, with the active site shuttling between Cu(I) and Cu(II). The Cu2+ in the oxidized state can accept one electron to form Cu1+ in the reduced protein. The geometry of the Cu center has a major impact on its redox properties. The Jahn-Teller distortion does not apply to the blue copper proteins because the copper site has low symmetry that does not support degeneracy in the d-orbital manifold. The absence of large reorganizational changes enhances the rate of their electron transfer. The active site of a type-I blue copper protein. Two 2-histidines, 1 methionine and 1 cysteine present in the coordination sphere. Example for Type-I blue copper protein are plastocyanine, azurin, and nitrite reductase, haemocyanin and tyrosinase.
The Blue Copper Proteins, a class of Type 1 copper proteins, are small proteins containing a cupredoxin fold and a single Type I copper ion coordinated by two histidine N-donors, a cysteine thiolate S-donor and a methionine thioether S-donor.[7] In the oxidized state, the Cu+2 ion will form either a trigonal bipyramidal or tetrahedral coordination. The Type 1 copper proteins are identified as blue copper proteins due to the ligand to metal charge transfer an intense band at 600 nm that gives the characteristic of a deep blue colour present in the electron absorption spectrum.[8] The protein structure of a Type 1 blue copper protein, amicyanin, is built from polypeptide folds that are commonly found in blue copper proteins β sandwich structure.[9] The structure is very similar to plastocyanin and azurin as they also identify as Type 1 copper proteins. They are also similar to one another due to the geometry of the copper site of each copper protein. The protein azurin has a trigonal bipyramidal geometry with elongated axial glycine and methoinione sulfur ligands. Plastocyanins have an additional methionine sulfur ligand on the axial position. The main difference of each copper protein is that each protein has different number and species of ligand coordinated to the copper center.
The strong bond between the copper ion and the cysteine sulfur allows for the non-bonded electron on the cysteine sulfur to be present on both the low/high spin state copper ion, dx2-dy2 orbital and the p-orbital of the cysteine sulfur. Most copper (II) complexes will exhibit the Jahn-Teller effect when the complex forms a tetragonal distortion of an octahedral complex geometry.[10] With blue copper proteins, a distorted tetrahedral complex will be formed due to the strong equatorial cysteine ligand and the weak axial methionine ligand. The two neutral histidine ligands are positioned by the protein ligand so the geometry is distorted tetrahedral. This will cause them not to be able to coordinate perfectly as tetrahedral or a square planar.
Lowering the temperature may change the transitions. The intense absorbance at about 16000 cm−1 was characterized the absorptions feature of blue copper. There was a second lower energy feature band with moderate absorption intensity. Polarized signal-crystal absorption data on plastocyanin showed that both bands have the same polarization ratio that associated with Cu(II)-S(Cys) bond. This is explained that the normal cupric complex has high energy intense sigma and low energy weak π bonds. However, in the blue copper protein case have low energy intense sigma and high energy weak π bonds because CT intensity reflects overlap of the donor and acceptor orbitals in the CT process. This required that the 3d(x2-y2) orbital of the blue copper site be oriented such that its lobes bisect the Cu-S(Cys) bond giving dominant π overlap with sulfur directly. Finally, the nature of the ground state wave function of the blue copper protein is rich in electron absorption spectrum.
The cysteine sulfur copper (II) ion bonds range from 2.6 to 3.2 Å.[11] With the reduced form, CuI, protein structures are still formed with elongated bonds by 0.1 Å or less. with the oxidized and reduced protein structures, they are superimposable. With amicyanin, there is an exception due to the histidine being ligated and it is not bound to copper iodide. In azurin, the Cysteine112 thiolate accepts the hydrogen bonds from the amide backbone of Asparagine47, and Phenylalanine114, and Histidine46 donates a hydrogen bond to the carbonyl backbone of Asparagine10. The Cysteine84 thiolate of plastocyanin accepts a hydrogen bond from a amide backbone, Asparagine38, and Histidine37 interacts strongly with the carbonyl backbone of Alanine33 and more weakly with the carbonyl backbone of Leucine5, Glycine34, and the amide backbone of Phenylalanine35.
Cu2+ complexes often have relatively slow transfer rates. An example is the Cu2+/+ aquo complex, which is 5 x 10−7 M−1.sec−1 compared to the blue copper protein which is between 1ms and 01μs.[12] Upon electron transfer the oxidized Cu2+ state at the blue copper protein active site will be minimized because the Jahn-Teller effect is minimized. The distorted geometry prevents Jahn-Teller distortion. The orbital degeneracy is removed due to the asymmetric ligand field. The asymmetric ligand field is influenced by the strong equatorial cysteine ligand and the weak axial methionine ligand. In Figure 2, an energy level diagram shows three different relevant geometries and their d-orbital splitting and the Jahn-Teller effect is shown in blue. (i) shows the tetrahedral geometry energy level diagram with a that is degenerate. The tetrahedral structure can undergo Jahn-Teller distortion because of the degenerate orbitals. (ii) shows the C3v symmetric geometry energy level splitting diagram with an 2E ground state that is degenerate. The C3v geometry was formed by the elongated methionine thioether bond at the reduced site. The unpaired electrons leads to the Jahn-Teller effect. (iii) shows the ground state energy level splitting diagram of the Cs geometry with a longer thioester bond and a subsequently shorter thiolate bond. This is the proper geometry of the blue copper protein. This shows that there is no presence of the Jahn-Teller effect. The energy diagram shows that the asymmetry of the short Cu-S(Cys) bond and the highly distorted Cu-L bond angles causes the degeneracy of the orbitals to be removed and thereby removing the Jahn-Teller effect, which is due to the weak donor at an Cu-S(Met) and strong donor at Cu-S(Met).