2⁢RG⁡(t02,t02+θ⁢c02,t02+θ⁢a02)=(t02+θ⁢∑m=0∞2m-1⁢cm2)⁢RC⁡(T2+θ⁢M2,T2)+h0+∑m=1∞2m⁢(hm-hm-1).