Förster resonance energy transfer (FRET) has been widely used in biological and biomedical research because it can determine molecule or particle interactions within a range of 1-10 nm. The sensitivity and efficiency of FRET strongly depend on the distance between the FRET donor and acceptor. Historically, FRET assays have been used to quantitatively deduce molecular distances. However, another major potential application of the FRET assay has not been fully exploited, that is, the use of FRET signals to quantitatively describe molecular interactive events. In this review, we discuss the use of quantitative FRET assays for the determination of biochemical parameters, such as the protein interaction dissociation constant (K d ), enzymatic velocity (k cat ) and K m . We also describe fluorescent microscopy-based quantitative FRET assays for protein interaction affinity determination in cells as well as fluorimeter-based quantitative FRET assays for protein interaction and enzymatic parameter determination in solution. Quantitative FRET analysisThe phenomena and principles of FRET were first discovered in 1948. In groundbreaking studies in the early 1970s, the quantitative relationship between FRET efficiency and the orientation and overlapping spectrum of the two fluorophores was described in biological macromolecules. This finding established the use of FRET as a spectroscopic ruler and bioanalytic tool [1][2][3][4][5][6] . Since then, FRET-based techniques have been extensively used in biological research in various settings to identify molecular interactive events in vitro and in vivo [7][8][9] . The FRET signal strength is generally determined by two major factors: the intrinsic FRET efficiency (E) of the donor and acceptor and the amounts of the interactive donor and acceptor. Moreover, the FRET efficiency depends strongly on the distance between the two fluorescent moieties, and this property is often used to measure the distance between donor and acceptor. The FRET efficiency is represented by the following:where R 0 is the Förster radius, the distance between donor and acceptor chromophores, when the efficiency of energy transfer is 50%, andÅ where Q 0 is the quantum yield of the donor chromophore in the absence of acceptor and n is the refractive index of the medium. The orientation factor (κ 2 ) depends on the relative orientation of the donor and acceptor dipoles and is given by the following:where α is the angle between the donor and acceptor transition moments, β is the angle between the donor moment and the line joining the centers of the donor and acceptor, and γ is the angle between the acceptor moment and the line joining the centers of the donor and acceptor. J is the spectral overlap integral, which is calculated as follows:where F(λ) is the fluorescent intensity of the donor chromophore at wavelength λ and is the molar extinction coeffi-