... Z1 - NG - K- Zootom'ical , ZI - T - M - KI Gr - Fr Zoot / omist , Z1 - T - Mst Zincograph'ic , Z1 - NG - K- Zoot'omy , Z1 - T - M Zincograph'ical - ly , Z. Zincog'raphy , Z1 - NG - K- Zos'tera , Zs1 - T - R Zinc'ous , Z3 - NG - KS ...
... Z1 need not have absolute calibra- tions as long as they give an accurate measure of the quantity involved . The essential requirement for accurate measurement is constancy of valve conditions ; and , as it is impossible to prevent ...
... Z1 cosh Pılı – x ) + Z sinh P1 ( − 2 ) Eo - Z1 sinh Pili + Z cosh Pili ( 32 ) ( Z1 + Z ) ePıllı −x ) + ( Z1 − Z ) e - P11 - x ) Eo - ( 42 ) Ix = Zi - . ( 43 ) Zi 1 whence Io - IB = ( 44 ) Z1 The sum of the backward trains is IBD = i1 ...
... Z1 c = Z1- Z Z1 + Z e - 2Pili · whence The sum of all the forward trains at B is Substituting this value of i in ( 40 ) we get : ( 32 ) Ix = IBf - i + ci + ci2 + .... . . , etc. = i / ( 1 - c ) . ( 33 ) or The sum of the backward trains ...
... Z1 ) and the drop in potential from d to c is this current times W5-6 , or E ( Z1 + Z2 + Z ̧ + Z4 ) W5-6 Z6 ( Z1 + Z2 + Z3 + Z1 ) + ( Z1 + Z2 ) ( Z3 + Z1 ) 2 The current through branches 3 and 4 is E ( Z1 + Z2 ) 1 ZË ( Z1 + Z2 + Zg + Z1 ) + ...
... Z1 ) 2 and the drop in potential from d to c is this current times W5-6 , 1 4 E ( Z1 + Z2 + Z3 + Z1 ) W5-6 Z6 ( Z1 + Z2 + Z3 + Z1 ) + ( Z1 + Z2 ) ( Z3 + Z1 ) The current through branches 3 and 4 is E ( Z , + Z , ) Z6 ( 21 + Z2 + 23 + Z1 ) + ...
... Z1 X2X3 ,Z1, X2 associated with the nodes 5, 9, 10, 1 on the edge e2. The possible values of Z1 ,X2, and X3 are ±1. Since the observables Z1 ,X2, and X3 all commute (because they refer to different qubits), the value of the observable ...