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B14
,\sinh{\left(\tau_{\textrm{CP}}E_2\right)} = i \sin{\left(\tau_{\textrm{CP}}|E_2|\right)}
</math>
The term <math>p_D</math> is based on product of the off diagonal elements in the CPMG propagator (Supplementary Section 3).
Equation 50 reads
<math>
R_{2,\textrm{eff}} = \frac{R_2^A+R_2^B+k_{\textrm{EX}}}{2}-\frac{N_{\textrm{CYC}}}{T_{\textrm{rel}}}\cosh{}^{-1}(v_{1c}) - \frac{1}{T_{\textrm{rel}}}\ln{\left( \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2k_{\textrm{AB}}p_D \right)} \\
= R_{2,\textrm{eff}}^{\textrm{CR72}} - \frac{1}{T_{\textrm{rel}}}\ln{\left( \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2k_{\textrm{AB}}p_D \right)}
</math>
=== Equation compared to Carver Richards 72 ===
[http://www.nmr-relax.com/manual/Dispersion_model_summary.html Please see the relax summary of the model parameters here.]