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An application of EPR spectroscopy that is becoming increasingly important is the measurement of distances between electron spins. Several EPR methods have been developed for this purpose, all based on measuring the dipolar coupling between two spins. Due to the specific nature of the sample, we applied dipolar relaxation enhancement measurements to study the geometry of a protein-protein complex. The paramagnetic centers in question had EPR spectra that were too broad and had such short relaxation time that they could not be studied using the more straightforward PELDOR technique. EPR spectral resolution can be increased appreciably by measuring at a frequency higher than conventional X-band (9 GHz) frequency. The spectra of many paramagnetic species can only be resolved at frequencies higher than 90 GHz. For accurate measurement of the orientation of the vector between two dipolar coupled spins with respect to the g-tensors of the spins, high spectral resolution is required. We therefore performed our EPR measurements at G-band (180 GHz) frequency. Dipolar relaxation measurements were applied to study the complex that is formed by the two electron-transfer proteins cytochrome c and cytochrome c oxidase (CcO) from the soil bacterium Paracoccus denitrificans. We were able to detect dipolar relaxation enhancement due to complex formation of soluble subunit II of P.d. CcO (CcOII) with two substrate cytochromes, which was practically absent in a mixture of CcOII with the negative control protein cytochrome c1. This complex formation was characterized by a pronounced temperature dependence that could be simulated using a home-written computer program. The G-band EPR measurements could not be simulated with a single complex geometry. This provided evidence for the hypothesis that electron-transfer protein complexes are short-lived and highly dynamic; they do not seem to form one specific electron-transfer conformation, but rather move around on each other’s binding surfaces and transfer an electron as soon as the distance between donor and acceptor is short enough. As a test of our simulation program, we also applied dipolar relaxation measurements to specially synthesized organic molecules that contained a nitroxide radical and a metal center. The transverse relaxation of Cu2+-OEP-TPA was compared to the relaxation of Ni2+-OEP-TPA at temperatures between 20 and 120 K. In this temperature range, the nitroxide relaxation was enhanced due to the presence of Cu2+, but not by Ni2+. Similarly, relaxation enhancement was found in the nitroxide-Mn2+ pair in Mn2+-terpyridine-TPA with respect to the terpyridine-TPA ligand. Due to the fast T2 relaxation of the nitroxide radical at high temperatures, the measurements were all performed in the low-temperature regime where the T1 relaxation rate of the metal ion was smaller than the dipolar coupling frequency. In this region, no structural information about the molecule can be deduced, since the dipolar relaxation enhancement is only determined by the T1 of the metal ion. The dipolar relaxation measurements we performed at high field indicated a difference in relaxation times between X-band and G-band frequencies. Extensive T1 - measurements of different paramagnetic centers (CuA, Cu2+) confirmed a strong dependence of T1 on magnetic field in the temperature range where the direct process is the dominating T1 relaxation process. This dependence is very strong (factor of 103 with respect to X-band), but does not follow the B04 dependence predicted in literature. The T1 relaxation of low-spin iron in cytochrome c at high magnetic field, estimated from dipolar relaxation data, is also in agreement with a larger contribution by the direct process (factor of 104). Dipolar relaxation enhancement was found to be a technique that is useful for measuring distances between paramagnetic centers, but only for systems where several important conditions are met, such as: the system exists in one certain static geometry, and the relaxation rate of the fast-relaxing spin is faster than the dipolar coupling frequency within the accessible temperature range. Additionally, it is a great advantage for the analysis of dipolar relaxation data if the procedure of dividing the relaxation trace of the dipolar-coupled slow-relaxing spin by the relaxation trace of the slow-relaxing spin in absence of dipolar coupling can be applied. Another useful application of dipolar relaxation enhancement measurements is the measurement of T1 relaxation of extremely fast-relaxing spins, or spins that are otherwise difficult to detect.