# Mx Sentence Examples

**Mx**, Maxilla.**Mx**, Maxilla.- N - '8'
**mx**, Maxillary. **Mx**, Maxillary.- Oe, Gullet; op, optic nerve; sb, sub-oesophageal ganglion; mn,
**mx**,**mx**', nerves to jaws; t, tentorium. - Oe, Gullet; op, optic nerve; sb, sub-oesophageal ganglion; mn,
**mx**,**mx**', nerves to jaws; t, tentorium. - The three pairs --
**Mx**2 of legs appear very early as rudiments. - ,?, VI B, Ventral view of the prosoma and of the first somite of the opisthosoma, with the appendages I to VI cut off at the base; a, tracheal stigma;
**mx**, maxillary processes of the coxae of the 3rd pair of appendages; g,genital aperture. - Thus sin e +sin 0=2 sin 2(0+x) cos 2(0-0) =
**mX**/(a +d) (5). - In the present application 4' is not necessarily equal to; but if P correspond to a line upon the grating, the difference of retardations for consecutive positions of P, so far as expressed by the term of the first order, will be equal to
**mX**(m integral), and therefore without influence, provided v (sin 0-sin0') = nzX (11), where a denotes the constant interval between the planes containing the lines. - Be produced by the continued multiplication of this series
**mX**m - I X 7n-2 X m-3... - X P11,1x, premaxilla;
**Mx**, maxilla; Ma, malar; Fr, frontal; L, lachrymal; Pa, parietal; Na, nasal; Sq, squamosal; Ty, tympanic; ExO, exoccipital; AS, alisphenoid; OS, orbito-sphenoid; Per, mastoid bulla. - In this simple case the temperature cycle at a depth x is a precisely similar curve of the same period, but with the amplitude reduced in the proportion rn ', and the phase retarded by the fraction
**mx**/27r of a cycle. - The wave at a depth x is represented analytically by the equation 0 - 0 0 = Ae
**mx**sin (21rnt -**mx**). **Mx**, 1st maxilla.- ., (X,., y,., z,.), the mass-centre (x, y, 1) is determined by the formulae _~(
**mx**) ~(my) ..E(mz) ~6 ~ ~(m) Y ~(m) Z ~(m)~ - If the co-ordinate axes coincide with the principal axes of this quadric, we shall have ~(myz) =0, ~(mzx) =0, Z(
**mxy**) = 0~ (24) and if we write ~(**mx**) = Ma, ~(my1) = Mb, ~(mz) =Mc2, (25) where M=~(m), the quadratic moment becomes M(aiX2+bI,s2+ cv), or Mp, where p is the distance of the origin from that tangent plane of the ellipsoid ~-,+~1+~,=I, (26) - For if the line in question be the axis of y, the first process gives us the values of
**mx**, and the second the value of 2(**mx**.x) or Z(mx2). - ~(
**mx**)_~(**mx**)=~(m)~i .4 - This leads, by the principles of 8, to the equations ~(
**mx**)=X, ~(mg.i) =Y,~(ml) =Z, I Z{m(yIzAi)}=L, ~(m(z~tx~i)} = M, ~(m(xpy~t)~ = N, - Since the reactions on the bearings must be statically equivalent to the whole system of effective forces, they will reduce to a force (X Y Z) at 0 and a couple (L M N) given by X=w~(
**mx**) =ai1~(m)~, Y =w1~(my) =wIï¿½(m)y, Z =0, L=wfZ(myz), M =, 2~(mzx), N =0, (8) **Mx**l,**Mx**2, 1st and 2nd maxillae.**Mx**., Maxilla.**Mx**REVOLUTIONARY EpocH, THE REACTION, AND THE**Mx**l, First maxilla.**Mx**2, Second maxilla.**Mx**', First and second pairs of maxillae.**Mx**, Maxilla.**Mx**, Part of the internal wood.- Hy, Hyoidean cornu
**Mx**, Maxilla.