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With amines, there is extremely rapid inversion in which the two configurations are interconverted.
Figure 10 compares the efficiency for the two configurations.
Barbour and Bertotti define an 'intrinsic difference' parameter that measures how different the two configurations are.
As shown in Equation 11, the parameters of the two configurations are nearly the same.
The null hypothesis states that there is no difference between the two configurations.
The procedure will be applied to the two configurations described in Section 2.1.
The reference axes and the irradiation position are reported in the two configurations.
It is very interesting that the trends for the two configurations are completely different.
During the suction phase the saddle point shows a different behavior in the two configurations.
The maximum power output and efficiency of the two configurations under different given conditions are analyzed.
It is shown that the same trend could be observed for the two configurations.
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