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  1. Start with true UTRs 
    LaTeX Math Inline
    body\displaystyle p_{u, ik}(t)
    with the same LTR asymptotic
    LaTeX Math Inline
    body\displaystyle p_{u, ik}(t) \rightarrow \frac{t}{RS}
    .
  2. Select injector W0 
    1. Select producer W1
      1. Perform two convolution tests to account for the impact from {W2 .. WN} production on to DTR_11
        LaTeX Math Inline
        bodyp_{u, 11}(t)
         and CTR_01
        LaTeX Math Inline
        bodyp_{u, 01}(t)
        :
        • Test #1 – DTR_11
          • Calculate historically-average rate for each producer: 
            LaTeX Math Inline
            body\displaystyle q^*_k = \frac{1}{N_k} \sum_{m=1}^{N_k} q_k(t_m)
          • Calculate interfering DTR_11: 
            LaTeX Math Inline
            body\displaystyle p^*_{u, 11}(t) = p_{u, 11}(t) + \sum_{k \neq 1} p_{u, k1}(t) \cdot q^*_k(t)
            , meaning that injector W0 is shut-down and all producers are working with constant rates 
            LaTeX Math Inline
            bodyq^*_k
            , except producer W1 which is working with unit-rate
        •  Test #2 – CTR_01Calculate historically-average rate for each producer: mathinline
          • body\displaystyle q^*_k = \frac{1}{N_k} \sum_{m=1}^{N_k} q_k(t_m)
            Calculate interfering CTR_01: 
            LaTeX Math Inline
            body\displaystyle p^*_{u, 01}(t) = p_{u, 01}(t) + \sum_{k} p_{u, k1}(t) \cdot q^*q_k(t)
            , meaning that injector W0 is working with unit-rate and all producers are working with constant rates 
            LaTeX Math Inline
            bodyq^*_k
      2. Calculate injection share constant
        LaTeX Math Inline
        body\displaystyle f_{01} = \frac{\dot p^*_{01}(t)}{\dot p^*_{11}(t)} \Bigg|_{t \rightarrow \infty}
         as LLS over equation: 
        LaTeX Math Inline
        body\displaystyle \dot p^*_{01}(t) = f_{01} \cdot \dot p^*_{11}(t)
    2. Repeat the same for other producers (starting from point 2a onwards)
  3. Repeat the same for other injectors (starting from point 2 onwards)

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