Abstract
The object of the earlier parts of this paper is to obtain relations connecting what Halphen calls the canonical invariants of the curve, without the intervention of what are called by him the fundamental invariants. In any geometrical investigation it is the canonical invariants which present themselves, and the relations between the consecutive canonical invariants, and the values of their differential coefficients must, if the method of investigation is to be used, be expressed, in terms of canonical invariants only, without the intervention of the other series of invariants which Halphen treats as fundamental.
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