ELEC 5564 Electric Power Generation by Renewable Sources - Shading Losses and Mitigation

Shading Losses

  • Shading from trees, buildings, clouds, other panels, or dust can significantly reduce the output of a solar cell.
  • Partial shading is a major cause of energy generation losses in photovoltaic (PV) systems.
  • Even a small shaded section can significantly reduce the performance of the entire solar photovoltaic panel.
  • Past studies have used a shading factor, assuming a proportional decrease in power production to shaded area and solar irradiance; while true for a single cell, this is not always accurate at the module or array level.

Affect of Shading on PV Performance

  • Figure A shows the P-V characteristics of a PV module.
  • Figure B shows the P-V characteristics of a PV module under partial shading.
  • The highest point in Figure A represents the Maximum Power Point (MPP).
  • For maximum power utilization, solar PV panels should operate at MPP.
  • Under uniform irradiance, the P-V characteristics exhibit one peak, representing a global and local MPP.
  • Multiple peaks can result from partial shading.

Hot Spot Heating

  • Figure A illustrates single-cell partial shading in an array.
  • Figure B shows the effect of one shaded cell in a PV module, which reduces the current through healthy cells, causing them to produce higher voltages that can reverse bias the shaded/faulty cell.
  • Hot spot heating occurs when the operating current exceeds the reduced ISCI_{SC} (short-circuit current) of a shadowed or faulty cell.
  • The affected cell or group of cells is forced into reverse bias, and the entire generating capacity will be dissipated in the shaded/faulty cell.
  • This power dissipation in a small area results in local overheating, or "hot-spots", leading to destructive effects like cell or glass cracking, melting of solder, or degradation of the solar cell.

By-pass Diodes

  • The effects of hot-spot heating can be mitigated using a bypass diode.
  • A bypass diode is connected in parallel, but with opposite polarity, to a solar cell.
  • Under normal operation, the bypass diode is reverse biased and acts as an open circuit.
  • If a solar cell is reverse biased due to a mismatch in short-circuit current between series-connected cells, the bypass diode conducts.
  • This allows current from the good solar cells to flow in the external circuit, rather than forward biasing each good cell.
  • The maximum reverse bias across the poor cell is reduced to about a single diode drop, limiting the current and preventing hot-spot heating.

Blocking Diode

  • A blocking diode prevents battery discharging through the PV modules.
  • When the battery voltage exceeds the generator voltage, the diode becomes reversely biased and blocks the discharging path.
  • It prevents current from flowing from one parallel string into a lower-current string, minimizing mismatch losses in parallel-connected arrays.
  • In larger PV arrays, individual PV modules are connected in both series and parallel.
  • An open-circuit in one of the series strings can cause a problem: current from parallel-connected modules will be lower than the remaining blocks (similar to the shading effect).
  • In parallel arrays with series-connected modules, the bypass diodes of the series-connected modules become connected in parallel. If the bypass diodes are not rated to handle the current of the entire parallel-connected array, this presents a problem.
  • To minimize mismatch losses, an additional diode, called a blocking diode, is used.

Series Connection - Under Inhomogeneous Conditions

  • Example: 36 cells connected in series, 35 are irradiated identically, but one is shaded by 75%.
  • The current through all cells is the same; the terminal voltage is determined by V=V<em>S(I)+35V</em>F(I)V = V<em>S(I) + 35V</em>F(I)
  • The module characteristic can be obtained by choosing a range of current.
  • V=V<em>1+V</em>2+=ΣVIV = V<em>1 + V</em>2 + … = \Sigma V_I
  • I=I<em>1=I</em>2=I<em>3=.=I</em>36I = I<em>1 = I</em>2 = I<em>3 = …. = I</em>{36}

Series Connection - Module Characteristic

  • Module characteristic when stopping at the short circuit current of the partially shaded cell.
  • Power reduces from 20.3 W to 6.3 W.
  • When current is higher, voltage of shaded cell becomes negative.
  • V=V<em>1+V</em>2+=ΣVIV = V<em>1 + V</em>2 + … = \Sigma V_I
  • I=I<em>1=I</em>2=I<em>3=.=I</em>36I = I<em>1 = I</em>2 = I<em>3 = …. = I</em>{36}

Series Connection - Cell Shading

  • Cell shading reduces the module output power drastically. In the example, module power reduces from 20.3 W to 6.3 W, although only 2% of the module surface is shaded.
  • The partially shaded cell operates as a load.
  • At higher irradiance, the power dissipated in the shaded cell further increases, heating the cell and causing hot spots, potentially destroying the cell.
  • To protect single cells from hot spot-related thermal damage, bypass diodes are integrated in parallel into the module.

Series Connection - Bypass Diodes

  • To protect single cells from hot spot related thermal damage, by- pass diodes are integrated in parallel into the module.
  • They are not active unless shading occurs.
  • 1 diode per 18-24 cells.

Solar P-V Characteristic

  • Depending on the degree of shading, the MPP shifts, and high losses occur despite integrated bypass diodes.
  • A 36-cell module with two bypass diodes.