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Förster Resonance Energy Transfer (FRET) between two fluorophore molecules can be used for studying protein interactions in the living cell. Here, a protocol is provided as to how to measure FRET in live cells by detecting sensitized emission of the acceptor and quenching of the donor molecule using confocal laser scanning microscopy.
Förster Resonance Energy Transfer (FRET) is the radiationless transfer of energy from an excited donor to an acceptor molecule and depends upon the distance and orientation of the molecules as well as the extent of overlap between the donor emission and acceptor absorption spectra. FRET permits to study the interaction of proteins in the living cell over time and in different subcellular compartments. Different intensity-based algorithms to measure FRET using microscopy have been described in the literature. Here, a protocol and an algorithm are provided to quantify FRET efficiency based on measuring both the sensitized emission of the acceptor and quenching of the donor molecule. The quantification of ratiometric FRET in the living cell not only requires the determination of the crosstalk (spectral spill-over, or bleed-through) of the fluorescent proteins but also the detection efficiency of the microscopic setup. The protocol provided here details how to assess these critical parameters.
Microscopy-based analysis of Förster Resonance Energy Transfer (FRET) permits assessment of interactions between proteins in live cells. It provides spatial and temporal information, including information on where in the cell and in which subcellular compartment the interaction takes place and if this interaction changes over time.
Theodor Förster laid the theoretical foundation of FRET in 19481. FRET is a radiationless transfer of energy from an excited donor to an acceptor molecule and depends upon the distance of the molecules and the relative orientation of their transition dipoles as well as the overlap between the donor emission and acceptor absorption spectra. The rate of energy transfer is inversely proportional to the sixth power of the donor-acceptor distance. Thus, FRET can be used to measure molecular proximity in the range of 1-10 nm.
FRET competes with other de-excitation processes of the donor molecule and results in the so-called donor-quenching and sensitized emission of the acceptor. Donor-quenching is a reduction of the number of emitted donor photons, while sensitized emission is an increase in emitted acceptor photons. Many microscopic FRET analyses use fluorescence intensity measurements, including acceptor photobleaching2, donor photobleaching2, or FRET-sensitized photobleaching of the acceptor3.
Here, a step-by-step experimental protocol and mathematical algorithm are presented to quantify FRET using donor quenching and acceptor sensitized emission4,5, a method often referred to as ratiometric FRET. Many protocols on how to approximate sensitized emission have been published, few have quantified the absolute FRET efficiency6,7,8,9. The quantification of FRET efficiencies in the living cell requires determining (i) the crosstalk (spectral spill-over, or bleed-through) of the fluorescent proteins and, also (ii) the detection efficiency of the microscopic setup. While crosstalk can be assessed by imaging cells expressing only one of the fluorophores, the assessment of the relative detection efficiency of the donor and acceptor fluorescence is more complicated. It requires the knowledge of at least the ratio of the number of donor and acceptor molecules giving rise to the measured signals. The number of fluorophores expressed in live cells varies, however, from cell to cell and is unknown. The so-called α factor characterizes the relative signal strengths from a single excited donor and acceptor molecule. Knowledge of the factor is a prerequisite for quantitative ratiometric FRET measurements in samples with variable acceptor-to-donor molecule ratios as encountered during live-cell imaging with fluorescent proteins. Using a 1-to-1 donor-acceptor fusion protein as a calibration probe permits the determination of the α factor and also serves as a positive control. This genetically coupled probe is expressed by cells in unknown total amounts but in a fixed and known relative amount of one-to-one. The following protocol lays out how to construct the 1-to-1 probe and how to use it for quantification of FRET efficiency. A spreadsheet that includes all formulae can be found in the supplement and can be used by the readers to enter their own measurements in the respective columns as outlined below.
While the protocol uses the GFP-Cherry donor/ acceptor pair, the presented approach can be performed with any other FRET pair. The Supplementary File 1 provides details on cyan-yellow pairs.
1. Plasmid construction
2. Cell culture and transfection
3. FRET Imaging
4. Image analysis for detecting absolute FRET efficiencies using donor quenching and sensitized emission
NOTE: Here, a practical step-by-step guide as to how to determine FRET efficiency with the use of the attached spreadsheet (Supplementary File 2) is provided. Theory and derivation of the presented equations can be found in detail in previous publications4,15,16,17. With the described settings, the following fluorescence intensities are collected.
Figure 1 shows the images obtained in the donor channel, channel 1 (488, 505-530 nm), the transfer channel, channel 2 (488, >585 nm), and the acceptor channel, channel 3 (561, >585 nm), respectively. Representative images of cells expressing GFP only, Cherry only, co-expressing GFP and Cherry, and expressing the GFP-Cherry fusion protein. The mean cellular FRET efficiencies calculated in NRK cells expressing GFP-Cherry fusion protein (positive co...
The presented protocol details the use of the genetically coupled one-to-one fluorescent protein calibration probe for quantifying FRET using the detection of sensitized emission of the acceptor and quenching of the donor molecule by confocal microscopy. This method can be applied to assess protein interactions in the physiological context of the living cell in different subcellular compartments. Spatial resolution can be further improved by applying the presented algorithm to calculate FRET efficiencies in each pixel of...
The authors have nothing to disclose.
We would like to thank the Neuroscience Imaging Service at Stanford University School of Medicine for providing equipment and space for this project. This research was supported by intramural funding of the Stanford Cancer Institute and the Gynecologic Oncology Division Stanford as well as GINOP-2.3.2-15-2016-00026, GINOP-2.3.3-15-2016-00030, NN129371, ANN135107 from the National Research, Development and Innovation Office, Hungary.
Name | Company | Catalog Number | Comments |
0.5% Trypsin-EDTA without phenol red (10x) | Thermo Fisher Scientific | 15400054 | |
Clontech mCherry N1 vector | Addgene | 3553 | |
DMEM without phenol red | Thermo Fisher Scientific | 11054020 | |
Fugene 6 | Promega | E2691 | |
HEPES | Thermo Fisher Scientific | 15630080 | |
LabTek 8-well chambers #1.0 | Thermo Fisher Scientific | 12565470 | |
L-Glutamine (200 mM) | Thermo Fisher Scientific | 25030081 |
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