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Open energy-system models are energy-system models that are open source. [a] However, some of them may use third-party proprietary software as part of their workflows to input, process, or output data. Preferably, these models use open data, which facilitates open science.
The SET rate follows the inverse of the fourth power of the distance [2] = where is the donor emission lifetime; is the distance between donor-acceptor; is the distance at which SET efficiency decreases to 50% (i.e., equal probability of energy transfer and spontaneous emission).
[1] [2] [3] The wheeling provider, or utility, receives compensation for the service and for electricity losses incurred in the transmission. As an economic concept, wheeling combines the traits of opposing designs of the electricity market: as a regulated public utility and a competitive market. [1] Two types of wheeling are:
In a spark gap Tesla coil, the primary-to-secondary energy transfer process happens repetitively at typical pulsing rates of 50–500 times per second, depending on the frequency of the input line voltage. At these rates, previously-formed leader channels do not get a chance to fully cool down between pulses.
Should an ideal transformer convert high-voltage, low-current electricity into low-voltage, high-current electricity with a voltage ratio of (i.e., the voltage is divided by and the current is multiplied by in the secondary branch, compared to the primary branch), then the circuit is again equivalent to a voltage divider, but the wires now have ...
The Dexter energy transfer rate, , is indicated by the formula: = ′ [] where is the separation of the donor from the acceptor, is the sum of the Van der Waals radii of the donor and the acceptor, and ′ is the normalized spectral overlap integral, where normalized means that both emission intensity and extinction coefficient have been adjusted to unit area.
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This transfer of energy between different scales requires that the dynamics of the system is nonlinear. Strictly speaking, a cascade requires the energy transfer to be local in scale (only between fluctuations of nearly the same size), evoking a cascading waterfall from pool to pool without long-range transfers across the scale domain.