There is a third type in which two dissimilatory excitations interfere with each other. Fortunately there is a great amount of experimental data at our command so that today we have a clear understanding of the essential points of the conditions necessary for the development of summation of excitation on the one hand, and inhibition on the other. If we take an instance of a momentary dissimilatory excitation operating upon an aërobic system in metabolic equilibrium, it is necessary to recall the two effects thereby produced. The stimulus brings about an oxydative decomposition of the living substance. Likewise there is a reduction of irritability. Both of these alterations are the foundation of interference. Both processes have a specific time of occurrence. The disintegration, determined by energy production, reaches a maximum suddenly, then diminishes, at first rapidly, then more and more slowly until the zero point is reached. In an analogous manner the irritability abruptly reaches a minimum, then increases rapidly, then more slowly, until it again reaches its previous value. When we represent these processes by a curve, they assume the following form. (Figure 47.) In this diagram the abscissa is the time, the ordinate value zero is the level of the metabolism of rest and the specific irritability. The points above the abscissa represent disintegration, that is, energy production, those under the abscissa, the reduction of irritability. A consideration of the latent period may be omitted. At the end of the curve the effect of stimulation may be assumed to have disappeared and the state of metabolic equilibrium reestablished. If we base our further observations upon this curve of excitation, we can study in them the factors upon which responsivity is dependent when a second exciting stimulus is operative during the course of the first. [Illustration: Fig. 47.] [Illustration: Fig. 48.] [Illustration: Fig. 49.] [Illustration: Fig. 50.]