I-V Characteristics of Photovoltaic cells

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Discussion Overview

The discussion centers on the I-V characteristics of photovoltaic (PV) cells, exploring their behavior under different load conditions, the relationship between voltage and current, and the implications of connecting PV cells to batteries. It encompasses theoretical and practical aspects of PV cell operation.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • Some participants inquire about the effects of a load resistance generating a higher voltage than that produced by a PV cell, questioning whether this affects the band gap.
  • One participant asserts that a load cannot generate a higher voltage than the PV cell, explaining that the operating point is determined by the intersection of the I-V curves of the load and the PV cell.
  • Another participant asks why current drops near the open circuit voltage (Voc), suggesting that current generation should depend on irradiance.
  • A response clarifies that at open circuit, the load resistance is effectively infinite, resulting in zero current.
  • One participant presents a scenario involving a 60W PV module connected to a 12V battery, questioning the implications of this setup on the PV module.
  • A reply indicates that while it is possible to connect the battery, it is not useful, as the battery would drain current through the PV module until the battery voltage drops to the PV module's maximum voltage.
  • Another participant suggests modeling the PV cell as a current generator with a diode, discussing the relationship between sunlight, knee voltage, and efficiency, particularly in different types of silicon.

Areas of Agreement / Disagreement

Participants express differing views on the implications of connecting PV cells to batteries and the behavior of current near the open circuit voltage. There is no consensus on the effects of load resistance exceeding the PV cell voltage or the optimal configurations for efficiency.

Contextual Notes

Some claims depend on specific assumptions about load conditions and the characteristics of different types of PV cells. The discussion includes unresolved questions regarding the interaction between PV cells and batteries, as well as the efficiency limits related to band gap and knee voltage.

vw_g60t
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Hi, could someone care to explain two things:

1) Whats happens when the resistance load of a circuit powered by a PV cell generates a higher voltage then that produced by the PV cell (does band gap get affected).

2) Why does current drop near the Open Circuit Voltage? Surely the generation of current depends on the irradiance on the PV cell? So why does current stop at the Voc point?

Example IV Charaeteristics of a typical photovoltaic cell:
http://www.tfp.ethz.ch/PV/HESC/IV.jpg

Thanks
 
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vw_g60t said:
Hi, could someone care to explain two things:

1) Whats happens when the resistance load of a circuit powered by a PV cell generates a higher voltage then that produced by the PV cell (does band gap get affected).

Well, actually that never happens. You can plot the i-v curve of a resistor on the same plot as the photovoltaic cell. It will be a straight line through the origin, with positive slope -- in accordance with Ohm's Law.

Where the two curves intersect will be the operating point for that particular load resistance. This happens in the "+v,+i" quadrant, so it will have voltage less than the open-circuit voltage and current less than the short-circuit current.

2) Why does current drop near the Open Circuit Voltage? Surely the generation of current depends on the irradiance on the PV cell? So why does current stop at the Voc point?

That's a general property of all power supplies. Open circuit means just that, i.e. the load resistance becomes (for all practical purposes) infinite. i=v/R=v/∞=0

Incidently, the i-v curve of a photovoltaic cell is related to that of a diode. Take a diode's i-v curve and flip it about the v-axis (equivalent to defining the current's polarity in the opposite sense). Then shift the curve upward by an amount equal to the short-circuit current. Works for photodiodes as well as photovoltaic cells, as they are the same thing but with different applications.
 
Thanks Redbelly, most useful response I've had on this site.

Excuse me if I am being dumb, but say I have a 60W PV module with Vmax point of 9v and I have it connected to charge a 12v battery?

Is this possible? If it is than surely the 12v voltage from the battery will be going into the 9v PV module - would'nt this have an effect on the PV module>?
 
It is possible, though not useful. To put it simply, the battery will be drained as it runs current through the PV module, in the negative direction, until the battery voltage has dropped to 9V. This is assuming the possibly high current does not damage the PV module.

To explain this, imagine drawing the i-v of the 12V battery on the same plot as the PV's i-v curve. Where do the 2 curves intersect? At a negative current, and at 12V less the voltage drop due to the battery's internal resistance.

I know your graph did not show negative currents, but the full i-v curve does indeed extend to negative currents, as well as to negative voltages.
 
Another way to predict the behaviour of a photovoltaic cell is to model it by a current generator with a diode as a shunt. It's exactly the same as the shifted diagram described above, so pick the one you feel more comfortable with.

The current is proportional to sunlight. It is lost in the diode if the user tries to exploit the current at a voltage exceeding the diode's knee voltage. An optimum can be searched (more complicated electronics) if operating at the beginning of the knee.

As the current density (created by sunlight) is low, so is the knee voltage, especially with poly or amorphous silicon. With single-crystal silicon, one may hope some 0.45V or a bit more. This voltage drops by 2.1mV/K, an important effect.

Also, nearly every single photon of energy >1.12eV is converted in an electron (and a hole) in single-crystal silicon cells, but this electron is available at 0.45V and this limits the efficiency. Expensive materials with a "direct gap" like GaAs have a knee voltage closer to the gap energy, and this improves efficiency.

The next limit is that much of the Sun's power is in infrared, which silicon doesn't harvest. For that, a smaller bandgap would be better, but then more energetic photons are badly used because their electron is available at the small knee voltage. One solution is to stack several cell materials specialised on different wavelengths.
 

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