2016
DOI: 10.1109/jphotov.2016.2583779
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<italic>In-Situ</italic> Monitoring of Moisture Ingress in PV Modules Using Digital Humidity Sensors

Abstract: A new in-situ moisture monitoring technique for PV modules is proposed using miniature digital humidity and temperature sensors. The sensors were embedded in three different ethylene-vinyl-acetate (EVA) stacks and proved to be resistant to lamination conditions. The fact that they are in direct contact to EVA does not affect their performance since their saturated relative humidity (RH) reading is proportional to the external RH in the air. By exposing the sensors to elevated temperature and RH conditions, wat… Show more

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Cited by 38 publications
(19 citation statements)
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“…In our humidity sensor experiments, and in similar experiments from the literature, it was seen that a nonzero initial concentration is present in EVA originating from diffusion from the atmosphere during warehouse storage prior to fabrication of the solar modules. For Fickian diffusion, the EVA properties are not affected by a nonzero C 0 , however the time required to reach saturation decreases with increasing C 0 .…”
Section: Finite Element Modelsupporting
confidence: 79%
“…In our humidity sensor experiments, and in similar experiments from the literature, it was seen that a nonzero initial concentration is present in EVA originating from diffusion from the atmosphere during warehouse storage prior to fabrication of the solar modules. For Fickian diffusion, the EVA properties are not affected by a nonzero C 0 , however the time required to reach saturation decreases with increasing C 0 .…”
Section: Finite Element Modelsupporting
confidence: 79%
“…In a G/G module, water is able to penetrate from the edges into the unprotected encapsulant. We solve the diffusion equation in a 2D domain of length L x and width L y equal to 0.2 m (ie, the size of a one‐cell mini‐module) using the Fourier series shown in Equation , an approach previously used by Kempe et al and Jankovec et al In the equation, c init and c surf are, respectively, the initial and the surface concentration of the encapsulant (g/m 3 ), and D its diffusion coefficient (m 2 /s). c(),,xyt=csurf+()cinitcsurf·16π2·n=012n+1sin()2n+1πxLxe2n+12π2Lx2italicDt··m=012m+1sin()2m+1πyLye2m+12π2Ly2italicDt …”
Section: Experimental Work and Modellingmentioning
confidence: 99%
“…The leakage current at negative biased modules was decreasing (exponential decay) over time to a more or less stable value. The current stabilizes when the EVA in the front and at the back of the cell is completely water soaked [16]. The leakage current of all four modules is presented in Figure 2.…”
Section: Leakage Currentmentioning
confidence: 98%