A horizontal

PHYSICS · Multi-part · Fermi University Physics · Earth, Climate & Energy Physics · Energy resources and conversion · Energy resources and conversion

Energy from Physics, Ch How efficient a solar cell can be: detailed balance, tandems and the field

Problem

A horizontal, 1 kWp1\,\mathrm{kWp} array of silicon modules (rated at 1000 W m−21000\,\mathrm{W\,m^{-2}}, 25∘C25^\circ\mathrm{C}) sits at latitude ϕ=52∘\phi = 52^\circ. Using the daily extraterrestrial insolation formula H0=24πS0[ωssin⁡ϕsin⁡δ+cos⁡ϕcos⁡δsin⁡ωs],ωs=arccos⁡(−tan⁡ϕtan⁡δ),\begin{aligned} H_0 &= \frac{24}{\pi}S_0\left[\omega_s\sin\phi\sin\delta + \cos\phi\cos\delta\sin\omega_s\right], \\ \omega_s &= \arccos(-\tan\phi\tan\delta), \end{aligned} with the solar constant S0=1361 W m−2S_0 = 1361\,\mathrm{W\,m^{-2}} and chapter 1's orbital factor (dˉ/d)2(\bar d/d)^2 set to one, take the summer solstice (δ=+23.4∘\delta = +23.4^\circ) and the winter solstice (δ=−23.4∘\delta = -23.4^\circ). Assume a clearness index KT=0.45K_T = 0.45 on both days, so H=KTH0H = K_TH_0 arrives at the ground on the horizontal plane, and ignore all other atmospheric and array losses except cell temperature. The module's power falls by 0.40%0.40\% per kelvin of cell temperature above 25∘C25^\circ\mathrm{C}. Take the mean daylight cell temperature to run 20 K20\,\mathrm K above the mean daylight ambient temperature, which is 18∘C18^\circ\mathrm{C} in summer and 5∘C5^\circ\mathrm{C} in winter, and assume this mean temperature derate applies throughout each day and that output otherwise scales linearly with irradiance. ((a)) Estimate the electrical energy generated per kWp\mathrm{kWp} on the summer solstice. ((b)) Estimate the electrical energy generated per kWp\mathrm{kWp} on the winter solstice.

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