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The temperature dynamic equation 

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anchordivT
 is going to be:

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anchorT1DTst
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\bigg( \sum_{a = \{w,o,g \}}\alpha \rho_\alpha \ c_{p \alpha} \ \mathbf{u}_\alpha \bigg) \  \nabla T 
  =frac{\partial T}{\partial l}
 \  =   \   \frac{1}{A}  \delta E_H}{ \delta V \delta t}\sum_\alpha \rho_\alpha \ c_{p \alpha} T_\alpha \frac{\partial  q_\alpha}{\partial l} 


The phase temperature 

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bodyT_\alpha
 is the temperature of the 
LaTeX Math Inline
body\alpha
-phase flowing from reservoir into wellbore.

It carries the original reservoir temperature with heating/cooling effect from reservoir-flow throttling and well-reservoir contact throttling:

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anchorTa
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T_\alpha = T_r + \epsilon_\alpha \, \delta P = T_r + \epsilon_\alpha \, (P_e - P_{wf})


The discrete computational scheme for 

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anchorTst
and its discrete computational scheme will be:

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anchorENA46
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\bigg( \sum_{a = \{w,o,g \}} \rho_\alpha^{k-1} \ c_{p \alpha}^{k-1} \ q_\alpha^{k-1} \bigg) T^{k-1} - \bigg( \sum_{a = \{w,o,g \}} \rho_\alpha^k \ c_{p \alpha}^k \ q_\alpha^k \bigg) T^k
 =   \sum_{a = \{w,o,g \}} \rho_\alpha^k \ c_{p \alpha}^k \ (q_\alpha^{k-1} - q_\alpha^k) \, (T_r^k + \epsilon_\alpha^k \delta p^k )

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