296 



K. HONDA : ON THE MUTUAL INFLUENCE 



TABLE VI. 



Here again, from Figs. G and 8 we observe that the intensity 

 of magnetization is, in this case, always less than that in the 

 former case for the same transverse and longitudinal fields, 

 so that the increase in weak longitudinal fields soon vanishes 

 when the transverse field is increased. 



Figs. 1, o and G show that in all longitudinal magnetiz- 

 ing fields less than Ob C.G.S. units, the magnetization increases 

 slowlv at first, and then rapidly, till it reaches a maximum. 

 Then the change of magnetization begins to decrease very slowly 

 in weak longitudinal fields, but rapidly in the stronger, and final- 

 ly becomes less than its initial value. The decrease of magneti- 

 zation in strong transverse or circular fields tends to approach 

 a certain limiting value as the field is increased. 



