In this view, the given equation is fair, if all the kernels of atoms participating in the synthesis are on one line. But actually, the directions of kernels movements participating in the synthesis of kernel «C» aren’t laid on one straight line, and leaning under different angels, as shown in figure № R-2.11.

  (20) Figure № R-2.11.

Therefore, must enter the coefficient accounting for the angle between the movement of nuclei before synthesis to the movement of the nucleus «C» after synthesis.

                                 β_j = Cosα_j

Where α_j — the angle between the movement directions of kernel j, before its participation in the synthesis, and kernel «C» received at the synthesis of kernel j.

The formula (2.44) with addition of factor β_j, will look:

Let’s consider the second addendum in the formula (2.43):

                                      Δm ^. c = P_I   

Where P_I — the impulse of radiation (or an impulse from radiation).

At the merge of kernels, the received kernel allocates energy in the form of radiation:

                                       E_I = Δm ^. c²    

Let’s consider this process more detailed. 

         (21) Figure № R-2.12.

The process of allocation of the radiation from kernel «C» during the synthesis, is represented In figure № R-2.12.
m_Ii, m_I1, m_I2, m_I3,… m_Ik – weights of each kind radiations allocated from a kernel «C» during its synthesis.
Defect of weight Δm, on the one hand is a difference of weights of kernels before the synthesis, and on the other hand — the sum of all weights of the radiations allocated as different kinds from kernel «C» at the synthesis:

In figure № R-2.12 it is evidently shown that radiation can be allocated in any party. Hence, it is necessary to enter the angular factors considering the corners actions of impulses from the radiations. 

                                 β_Ii=(Cos180⁰+α_Ii)                                                             (2.47a)

Where β_Ii — angular factor,

       α_Ii — the angle between direction of movement of a kernel «C» and  direction of the radiation.

On each radiation allocated from the kernel, there is a certain part of weight from Δm.

Hence, for each radiation it is necessary to enter the mass factor ε_Ii defining a share Δm going on a concrete radiation.

                                 m_Ii = ε_Ii ^. Δm

In the given view m_Ii shows, what part of the defect of weight Δm, is allocated as I-radiation from the kernel at moment of synthesis.

The mass factor ε_Ii for i-radiation is equal:

              (2.47b)

Every emission has its own speed, which is not always equal to the speed of light, so must enter the the rate coefficient s_Ii: 

             (2.47c)

v_Ii — speed of i radiation,

c — speed of light.

Proceeding from stated above, the second addendum (2.43) «Δm ^. c» will become the formula:

The second summand can vary from (-Δm ^. C) to (+ Δm ^. C), a negative value is taken when the pulses from the emission hinder nucleus. Zero — when the pulses from the radiation balance each other, or there is no energy release.

(+ Δm ^. C) — when all of the radiation have been allocated to one side and their impulses increased rate of the nucleus «C».

The primary goal that was established by us is the definition of speed and energy of kernel «C».

Whether these values are enough for the following act of synthesis?

From the formula (2.49) it is necessary to define the speed v_c of kernel «C». 

                                        (2.50)