358 FRAGMENTS OF SCIENCE. 



practical service whilst we are waiting for the actual 

 truth. 



The state of excitement into which iron is thrown 

 by the influence of a magnet, is sometimes called 

 ' magnetisation by influence.' More commonly, how- 

 ever, the magnetism is said to be ' induced ' in the iron, 

 and hence this mode of magnetising is called ' mag 

 rietic induction.' Now, there is nothing theoretically 

 perfect in Nature : there is no iron so soft as not to 

 possess a certain amount of coercive force, and no steel 

 so hard as not to be capable, in some degree, of mag- 

 netic induction. The quality of steel is in some 

 measure possessed by iron, and the quality of iron is 

 shared in some degree by steel. It is in virtue of this 

 latter fact that the unmagnetised darning-needle was 

 attracted in your first experiment ; and from this you 

 may at once deduce the consequence that, after the 

 steel has been magnetised, the repulsive action of a 

 magnet must be always less than its attractive action. 

 For the repulsion is opposed by the inductive action of 

 the magnet on the steel, while the attraction is assisted 

 by the same inductive action. Make this clear to your 

 minds, and verify it by your experiments. In some 

 cases you can actually make the attraction due to th< 

 temporary magnetism overbalance the repulsion due 

 the permanent magnetism, and thus cause two poles of 

 the same kind apparently to attract each other. When, 

 however, good hard magnets act on each other from 

 sufficient distance, the inductive action practically 

 vanishes, and the repulsion of like poles is sensibly 

 equal to the attraction of unlike ones. 



which are repelled by magnets. Like soft iron, such bodies 

 thrown into a state of temporary excitement, in virtue of whi< 

 they are repelled ; but any attempt to explain such a repulsion 

 the decomposition of a fluid will demonstrate its own futility. 



