Automatic compilation method and framework for generating a layout of integrated memory-compute circuit
US-2024403527-A1 · Dec 5, 2024 · US
US11550983B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11550983-B2 |
| Application number | US-201916682807-A |
| Country | US |
| Kind code | B2 |
| Filing date | Nov 13, 2019 |
| Priority date | Nov 14, 2018 |
| Publication date | Jan 10, 2023 |
| Grant date | Jan 10, 2023 |
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A method for determining an electrical model of a string of photovoltaic modules from a characteristic I(V) of the string includes detecting a first linear zone and a second linear zone of the characteristic I(V); initialising the parameters of a non-by-pass electrical model corresponding to a first operating condition, called a non-by-pass condition; optimising the parameters of the non-by-pass electrical model from a reference characteristic I(V ref ) equal to I(V), determining the parameters of the electrical model corresponding to a second operating condition, called a by-pass condition, in order to obtain a by-pass electrical model from the characteristic determining, from the characteristic I(V) the best model among the non-by-pass model and the by-pass model.
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The invention claimed is: 1. A method for determining an electrical model of a string of photovoltaic modules from a characteristic I-V of said string and a non-by-pass model corresponding to a first operating condition of the string, called a non-by-pass condition, given by the following equation: Y = I p h - W t h + R s × Y R p - I 0 × ( e W t h + R s × Y N - 1 ) with I ph the photocurrent, R s the series resistance, R p the parallel resistance, I 0 the dark current of the diode, N = k q × N s × T ideal with T ideal ∈[200,300], N s the number of series cells in the string, k b is the Boltzmann's constant and q is the elementary charge of a proton, Y the current passing through the string and W th the voltage across the string, I ph , R s , R p , I 0 and N being parameters of the non-by-pass model; and a by-pass model corresponding to a second operating condition of the string, called a by-pass condition and given by the following equation: W mod ( Y )= W 1 ( Y )+ W 2 ( Y ) with W mod the voltage across the string according to the by-pass model for the current Y, W 1 ( Y ) = ( 1 - P d ) × W t h ( Y ) and W 2 ( Y ) = P d × W t h ( Y 1 - P I ) where W th (Y) is the voltage across the string given by the non-by-pass model, P d the by-pass diode proportion and P I the short-circuit current loss proportion induced by the by-pass, Pa and Pi being parameters of the by-pass model, the method comprising: a step of detecting a first linear zone and a second linear zone of the characteristic I-V; a step of initialising the parameters of the non-by-pass electrical model from the characteristic I-V; a step of optimising the parameters of the non-by-pass electrical model from a reference characteristic I(V ref ) equal to I(V); a step of determining the parameters of the by-pass electrical model, in order to obtain a by-pass electrical model from the characteristic I-V; and a step of determining, from the characteristic I-V, a best model from the non-by-pass model and the by-pass model. 2. The method according to claim 1 , further comprising, before the step of detecting the linear zones of the characteristic I-V, a step of checking the data of the characteristic I-V. 3. The method according to claim 2 , wherein the step of checking the data of the characteristic I-V comprises at least one of both following sub-steps: a sub-step of detecting the switching period of the string, the data measured outside the switching period being removed; a sub-step of removing the outliers. 4. The method according to claim 1 , wherein the step of detecting a first linear zone and a second linear zone of the characteristic I-V comprises: a sub-step of determining the maximum power point (I MPP , V MPP ), the points of the characteristic I-V located above the straight line passing through the origin (0,0) and the point (I MPP , V MPP ) being considered as candidates for the first linear zone, and the points located below this straight line being considered as candidates for the second linear zone; a sub-step of determining the linear model of the current Y as a function of the voltage W across the string such that Y=a sc ×W+b sc from the candidate points for the first linear zone and the linear model of the voltage W across the string as a function of the current Y such that W=a oc ×Y+b oc from the candidate points for the second linear zone, so as to determine the parameters a sc , b sc , a oc and b oc . 5. The method according to claim 4 , wherei
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