A method for estimating radiated emission level from an EUT at an arbitrary position on the turn table at OATS, wherein said EUT is supposed as electric and magnetic dipole moments P(=Pxejψpxax+Pyejψpyay+Pzejψpzaz, where, ax, ay, az are respectively the unit vectors, in the directions of x, y and z) and M(=Mxejψmxax+Myejψmyeay+Mzejψmzaz) with initial phases to the respective components, and has a correlation with the GTEM cell output powers of [Equation 20] in order to compute vertical and horizontal radiation electric fields from the object on the ground plane of OATS or SAC ( a ) P z 2 + k 0 2 M y 2 = P 1 ( f ) + P 4 ( f ) 2 ( b ) P z 2 + k 0 2 M x 2 = P 3 ( f ) + P 5 ( f ) 2 ( c ) k 0 P z M y sin ( Ψ pz - Ψ my ) = P 4 ( f ) - P 1 ( f ) 4 ( d ) k 0 P z M x sin ( Ψ pz - Ψ my ) = P 5 ( f ) - P 3 ( f ) 4 ( e ) k 0 2 M x M y cos ( Ψ mx - Ψ my ) = P 2 ( f ) P 1 ( f ) + P 3 ( f ) + P 4 ( f ) + P 5 ( f ) 4 - 2 ( P 1 ( f ) + P 3 ( f ) - P 4 ( f ) - P 5 ( f ) ) 4 ( f ) P x 2 + k 0 2 M z 2 = P 6 ( f ) + P 9 ( f ) 2 ( g ) P x 2 + k 0 2 M y 2 = P 8 ( f ) + P 10 ( f ) 2 ( h ) k 0 P x M z sin ( Ψ px - Ψ mz ) = P 9 ( f ) - P 6 ( f ) 4 ( i ) k 0 P x M y sin ( Ψ px - Ψ mz ) = P 10 ( f ) - P 8 ( f ) 4 ( j ) k 0 2 M y M z cos ( Ψ my - Ψ mz ) = P 7 ( f ) P 6 ( f ) + P 8 ( f ) + P 9 ( f ) + P 10 ( f ) 4 - 2 ( P 6 ( f ) + P 8 ( f ) - P 9 ( f ) - P 10 ( f ) ) 4 ( k ) P y 2 + k 0 2 M x 2 = P 11 ( f ) + P 14 ( f ) 2 ( l ) P y 2 + k 0 2 M z 2 = P 13 ( f ) + P 15 ( f ) 2 ( m ) k 0 P y M x sin ( Ψ py - Ψ mx ) = P 14 ( f ) - P 11 ( f ) 4 ( n ) k 0 P y M z sin ( Ψ py - Ψ mx ) = P 15 ( f ) - P 13 ( f ) 4 ( o ) k 0 2 M x M z cos ( Ψ mx - Ψ mz ) = P 12 ( f ) P 11 ( f ) + P 13 ( f ) + P 14 ( f ) + P 15 ( f ) 4 - 2 ( P 11 ( f ) + P 13 ( f ) - P 14 ( f ) - P 15 ( f ) ) 4 . [Equation 20]