2. Physical bases of «analytical astrophysics»
Copyright © 2010 by Stanislav Kozlov
All rights reserved. No part of this book may be reproduced in any form or by any
electronic or mechanical means without permission in writing from the author.
2.5. Speed of kernels at synthesis
We know that for the synthesis of two kernels and more, it is necessary, that at least part of them will have kinetic energy and a speed sufficient for overcoming the coulomb barrier.
Where from a kinetic energy for synthesis appears in kernel?
Let’s consider the process we’re interested in on the example of three kernels: «A» and «B», which after the synthesis turning into a kernel «C». And this kernel «C» should participate in the following acts of synthesis.
Where from a kinetic energy for synthesis appears in kernel «C»?
It’s very simple, during the synthesis of kernels «A» and «B», their impulse is transferred to kernel «C», but at this act of synthesis, an energy in the form of radiation is allocated: