... n2zx n " x dt Wz W1 = + A A p.2 ( 1 + e ) r′2 } ( 210 ) dw3 = 0 ; dt Wz = n , ( 211 ) from the third of these if n ... n'2 zx n'2x + ; 2 ( 1 + e ) r ' and from these equations all the phænomena of the rotation are to be deduced ...
... N2zx = QIII.zx QI , zx - QIII.zx N1zx and N2zx , respectively , where N1zx function eikx + 14 ) = = ( a1 ) ell ( 12 ) -ikx e b2 the spin current becomes m { Re [ aja2 ] – Re [ b * b2 ] } , = k Qxx = Qyx = k Qzx = - 2m { ( 19112 – 1a212 ) ...
... n'2 zx n'2'x ' ) dt Wz W1 = + A A r.2 ( 1 + e ) r22 § ( 210 ) dw3 dt = 0 ; Wz = n , from the third of these ( 211 ) if n is the angular velocity of the earth about its polar axis of figure . Also , for convenience of expression , let C ...
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... on K1 ( N2 ) , define 1 υλ Ξ ( N2 ) 2 Σ λ ( k ( a , b ) ) ̄1ñ ( k ( a , b ) ) . v2 . a , bЄZ / N2Zx Here ø is Euler's function . Observe that the vector 5.3 Explicit realization of the action of GL ( 2 , A finite ) 171.
... N2zx ди zx Iz ( 80 ) where N2 , is the coefficient of eddy viscosity or turbulent viscosity , which , like molecular vis- cosity , has dimensions of M L - 1 T - 1 . The subscripts refer to eddy viscosity in the vertical direction ( z ) ...
... N2zx ( zxDz ) , ( 1 . 134 ) where the first term represents the motion of magnetization z around the effective magnetic field He ; the second term is the Gilbert dissipative term . Since the Landau - Lifshitz equations are important ...
... n2Zx › Z'zl2Xx + Mz Yz + ng Zx . ) . ( 8 ) On substituting from ( 7 ) in ( 8 ) , and taking account of ( 6 ) , we find formulæ of the type X'x = l3Xx + m23Y1 + n2 Z2 + 2m ̧n ̧ Y2 + 2n ̧l1⁄2Z ̧ + 211m , X , X'y = l1l2 X x + m2 m2 Yy + ...
... n2zx / r2inx ( x2 - r / c2 ) 12 / r2 . ( 15 ) ( 16 ) At this stage , the analysis of the complex p - plane is split into two cases : one , the velocity of the load is smaller than the velocity of S - waves ( v < cs ) and two , the ...
... n2zx Іх VH -1 H2 X2 ( b ) pu ZHX ti X1 pu I + pu VH pu VX H2 X2 ( c ) Fig . 7.1 . Single - phase , two - winding transformer equivalents : ( a ) equivalent in system quantities , ( b ) simplified equivalent with all series impedance ...