“…The solution of (16), and thus the solutions of (14), (12), and (9), constitutes the intermediate integral of the LB equation (1) in the phase plane. In other words, when obtaining the solution of the transformed equation (16) in the form = ( , * ), * = first integration constant, the solution of (14) becomes ( ) = − ( ), the solution of (12) is ( ) = − ( 4/3 ), and finally the solution of (8) is ( ) = − −1/3 ( 4/3 ). Thus, the solution to the original Langmuir equation 1in the physical plane can be obtained by the integration by parts of the following equation:…”