During nuclear fission, the binding energy of the initial nuclide, aka the educt, is converted into kinetic energy for the nuclei of the products and neutrons, as well as high-energy quanta ($\gamma$-photons) and other particles. At least that is the ideal process.
In reality, some energy is also "lost" in the form of Thermal Energy. This is known as Decay Heat. However, the Decay Heat does not have to be implied directly from the nuclear fission. While it contributes approximately 7% of the energy during operation, it continues to be produced after the fission process and energy conversion process is stopped as the daughter fragments continue to decay. This heat must still be removed. It does decrease with time; the initial predominant decay contributors have a 56 second half-life, resulting initially in the 7% reducing with approximately one hour half-life. Once those decays occur, at about 1% power, the reduction then asymptotically approaches zero over much, much longer period. Some sensible heat will still be released over many years, and some decay takes thousands of years, even though the heat contribution is insignificant.
The kinetic energy arises from the direct conversion of the binding energy. We can easily recognize this kinetic energy from the speed of the nuclei and neutrons. The $\gamma$-photons can also arise directly from the conversion of the binding energy. However, they can also from the further radioactive decay of the products. The products of nuclear fission can also decay radioactively and other particles such as $\beta^{-}$ (electrons), $\beta^{+}$ (positrons), neutrinos, ... But the starting material itself can also decay radioactively and therefore emit particles alongside these. However, this process itself is no longer part of Fission. However, it should not be forgotten that they also take kinetic energy from the initial nuclide.
Uranium-$235$:
Source |
Average energy released $\left[ \mathrm{MeV} \right]$ |
Instantaneously released energy: |
Sum: $180.9$ |
Kinetic energy of fission fragments |
$169.1$ |
Kinetic energy of prompt neutrons |
$4.8$ |
Energy carried by prompt $\gamma$-photons |
$7.0$ |
|
|
Energy from decaying fission products: |
Sum: $21.6$ |
Energy of $\beta^{-}$ particles |
$6.5$ |
Energy of delayed $\gamma$-photons |
$6.3$ |
Energy released when those prompt neutrons which do not (re)produce fission are captured |
$8.8$ |
|
|
Energy of anti-neutrinos |
$8.8$ |
Source: Wikipedia