Some authors suppose the electrostatic force acting on the electron or ion carrier as the force of material transference, but we can not concieve it. The authors suppose that prihcipal cause of the faulty conclusions described in some literatures are concerned with the incomplete photographs as illustrated in Fig. 1, Fig. 2.
Many papers discuss the pinch effect, but it is proved clearly by our previous paper that the short circuit breaks without the force of pinch effect, and therefore it is impossible to explain the material transference by the force of pinch effeet.
Larson's ingepeous experiment shows the particle form transference in the case of coated electiodes of cellulose and sodium silicate coating, but the authors suppose above experiment is of normal polarity but the phenomena in the case of a.c. or reversed polarity in which the electrode is used practicaly is very different as shown by our report. (Photographs No. 29-55).
Further discussions are described in the main report.
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