Oc. ' 'r.**bs** px, Premaxilla.

Let the determinant of the b's be Ab and B rs, the minor corresponding to b rs .

On this principle the covariant j is expressible in the form R 2 j =5 3 + **BS** 2 a+4ACSa 2 + C(3AB -4C)a3 when S, a are the above defined linear forms.

We will choose from the forms in such manner that the product of letters A is either a power of A i, or does not contain A i; this rule leaves us with A2B 1 B 2 and A 2 B,**Bs**; of these forms we will choose that one which in letters B is earliest in ascending dictionary order; this is A2B 1 B 21 and our earliest perpetuant is (22)a(21)b - (221)a(2)b, and thence the general form enumerated by the generating function Z7 is (1-z)(1 - z2)2 (2 A2+2) a (2ï¿½2 +1 1ï¿½1 +1) b - (2 A2+2 1)a (2 M2+1 1, ai)b ...

**Bs**, Blood sinus.

**Bs**, Blood sinus.

The diameter sought is the straight line from A to the limiting position of the series of B's, say the straight line AB co.

If the observer be stationary at B, the star will appear in the direction **BS**; if, however, he traverses the distance BA in the same time as light passes from the star to his eye, the star will A B appear in the direction AS.

I.; B's and Reinholds Briefwechsel.

Libation **bs**.t **bs** **bs** L vase it, cord on wz wz wz J stick ~J7 basket nb.t nb r~ looped ?

Hence set out the possible direction of **Bs** motion in the velocity diagram, namely cbi, at right angles to CB.

From this law it follows, for example, that equilibrium is never quite obtained for those presentations which continue above the threshold of consciousness, while the rest 1 Thus, taking the case above supposed, the share of the inhibendum falling to the smaller presentation b is the fourth term of the pro zab portion a+-b: a:: b: a + b; and so b's remainder is b - ad-b - a-f-b' which only =0 when a = oe .

**Bs**, **bs**,Bee spaces.

**Bs**, **bs**, Bee spaces.

Suppose B not to be fixed, but to be capable of moving against some third body C (which might, e.g., contain cylindrical bearings, if B were a drum with its shaft), itself fixed, - and further, suppose the frictional resistance between B and C to be the only resistance to B's motion.