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p_R(t) = p_{R,{\rm tr}}(t) - \delta p_R(t), \delta p_R(t) = \int_0^t p_{uGR}(t-\tau) \, dq_G(\tau)


The generator's flowrate history 

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bodyq_G(t)
, generator's wellbore pressure history 
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bodyp_{G,{\rm tr}}(t)
  and receiver's wellbore pressure history 
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bodyp_{R,{\rm tr}}(t)
  are assumed to be known for the whole period of the test. 


The result of decomposition is the set of the unit-rate transient responses, DTR

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body p_{uGG}(\tau)
 and CTR
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body p_{uGR}(\tau)
), which characterise reservoir properties round generator and between generator and receiver.

The pressure trends at generator 

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bodyp_{G,{\rm tr}}(t)
 and receiver 
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bodyp_{R,{\rm tr}}(t)
 may have unknown origin but in order for decomposition to work they should have minimum correlation with generating well pressure variation 
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body\delta p_G(t)
. In terms of spectral analysis this means that trend's spectrum contains minimum overlap with spectrum of pressure variation 
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body\delta p_G(t)
 at generator.

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