ordered couplesFor the future we follow the custom of omitting the sign wherever possible, thus stands for and for . , , and .
We have already proved that
Furthermore we now have
Hence both for addition and for multiplication the couple plays the part of zero in elementary arithmetic and algebra; compare the above equations with , and .
Again consider : this plays the part of in elementary arithmetic and algebra. In these elementary sciences the special characteristic of is that , for all values of . Now by our law of multiplication
Thus is the unit couple.
Finally consider : this will interpret for us the symbol . The symbol must therefore possess the characteristic property that . Now by the law of multiplication for ordered couples
But is the unit couple, and is the negative unit couple; so that has the desired property. There are, however, two roots of to be provided for, namely . Consider ; here again remembering that , we find, .
Thus is the other square root of . Accordingly the ordered couples and are the interpretations of in terms of ordered couples. But which corresponds to which? Does correspond to and to , or to , and to ? The answer is that it is perfectly indifferent which symbolism we adopt.
The ordered couples can be divided into three types, (i) the "complex imaginary" type , in which neither nor is zero; (ii) the "real" type ; (iii) the "pure imaginary" type . Let us consider the relations of these types to each other. First multiply together the "complex imaginary"
couple and the "real" couple , we find
Thus the effect is merely to multiply each term of the couple by the positive or negative real number .
Secondly, multiply together the "complex imaginary" couple and the "pure imaginary" couple , we find
Here the effect is more complicated, and is best comprehended in the geometrical interpretation to which we proceed after noting three yet more special cases.
Thirdly, we multiply the "real" couple by the imaginary and obtain
Fourthly, we multiply the two "real" couples and and obtain
Fifthly, we multiply the two "imaginary couples" and and obtain
We now turn to the geometrical interpretation, beginning first with some special cases.