Thursday, May 12, 2016

HW on Solar cells.

Please feel free to discuss your thoughts and results for these problems here. Let's have this due in class next Wednesday.  If you want to rush through 1-6 to get to 7 that would be fine. I think you already did a lot of this in class. Problem 7 and the extra credit part of 7 are the most interesting part, I think.

(For these problems, where it is relevant, let's assume a symmetric n-p junction doped to \(10^{17} cm^{-3}\) on either side.  [and to a semiconductor for which  \(E_g = 1 eV, \quad kT=.025 eV\) and \(D_c = D_V = 12 \times 10^{21} \frac{states}{eV*cm^3}, \quad B_c = B_V = 3 eV\)].)

Discussion question 1. In the ideal junction approximation, I believe that we found that for a junction connected to a battery of voltage V_a, the current density will have the form:
\(J(V_a) = J_o (-1 + e^{eV_a/kT})\)
Based on the calculation we did of the diffusion current at x_d, what is a reasonable estimate for the value of J_o? What are the units of J_o?

Discussion question 2. Consider an n-p junction with no bias voltage.  a) Suppose somewhere along "x" a photon excites an electron from the valence band to the conduction band. What do you think will happen to that electron?  Does it matter where that occurs?  b) Suppose there is a uniform flux of photons in the semiconductor and some of them excite electrons from the VB to the CB. What happens? c) What energy would you want that photon to be?

4. (Solar cell question) Suppose there is an incoming flux of 10^16 photons per second per cm^2 on a 1 cm^2 area junction. Suppose that 50% of them excite an electron from the VB to the CB. Suppose also that there is a wire connecting the far side of the n side to the far side of the p side.
a) What happens in the junction?
b) What happens in the wire?
c) What sort of assumption would you need to make in order to do a quantitive estimate of the current in the wire? What do you estimate that current to be?
d) What would the current be for an incoming flux of 10^17 photons/(sec*cm^2) on a 1 cm^2 area junction (suppose that 50% of them excite an electron from the VB to the CB).

5. (Solar cell- capacitor question) Suppose there is an incoming flux of 10^16 photons per second per cm^2 on a 1 cm^2 area junction. Suppose that 50% of them excite an electron from the VB to the CB. Suppose also that there is a capacitor in series with the junction. (no battery or resistor, just the capacitor).
a) After a long time, what is the equilibrium charge of the capacitor? How come? Explain your reasoning.
b) Do a sketch showing the junction, the circuit, and which side of the capacitor has positive and negative charge.
c) After a long time, what is the equilibrium charge of the capacitor for  a flux of 10^17 photons per second per cm^2?

6. Consider a junction (of area A) for which the current-voltage relationship without illumination is: \(I(V_a) = I_o (-1 + e^{eV_a/kT})\) where \(I_o\), which is associated with a bias voltage induced diffusion current, is \(I_o = 3 \times 10^{-11}\) coulombs/sec. (extra credit: Comment on whether or not this value of \( I_o\) seems reasonable based on your understanding of biased junction diffusion current (and problem 1).)
     Now suppose additionally that  the junction is illuminated by a flux of photons such that \(8 \times10^{16}\) photons/second are absorbed in the depletion region and each of those photons excites an electron from the VB to the CB which then is pushed over to the n side by the electric field in the depletion region.
a) suppose there is a wire connecting the n-side to the p-side. If we make the simplifying assumption that each of those excited electrons contributes to the current, then what is the current through the wire?
b) Consider that case where there is a capacitor in the wire (in series with the junction). What charge and voltage would the capacitor reach in steady state? (Asymptotically) Let's say C= 10 Coulombs per Volt.
c) What charge and voltage would the capacitor reach for \(10^{15}\) photons per second absorbed ?
d) What charge and voltage would the capacitor reach for \(10^{16}\) photons per second absorbed? How come this is not 10x as large?

7. This problem involves the same junction as in the previous problem, but with a resistor in series with it instead of a capacitor. Let's assume \(8 \times 10^{16}\) photons per second absorbed creating a current due to illumination.
a) With a resistance of 1 Ohm, can you get a pretty good estimate of the current through the circuit (to about 5% accuracy or better) without too much work? How come? What is I? What is the power, e.g., \(I^2 R\), generated in the resistor in this case? What about for R =: 2 Ohms, 4 Ohms, 8 Ohms and 32 Ohms. Plot power generated in the resistor as a function of R. Is the relationship linear?
b) What value of R would give you a voltage across the resistor of 90% of the voltage that you would  get with a capacitor (as in problem  6b). What is the power generated in the resistor for this case?
c) Is there a value of R that gives you the highest power generated in the resistor, (or would that just be infinity)? If there is such a value, what is it for this case?
d) extra credit. Make a table showing values of R, I, V and power generated. Cover an interesting range.
e) Special Extra credit: Compare the power of the incoming photons to the power generated in the resistor! Think about and discuss conservation of energy, where energy goes in this process, etc! (Send me a pdf or post here anything you get.)

4 comments:

  1. To get things started, in office hours last week we discussed how the current from photons exciting electrons into the conduction band is only HALF the total current because of the holes left in the valance band which also migrate but in the opposite direction. So in total we should have 1 current from the electrons moving to the left and a 2nd current from the holes moving to the right (which can be thought of as electrons moving to the left). What do you guys think? Is this right? Let me know, thanks.

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  2. For question 2 part b we have come to the conclusion that there is current all over. I can see how there is current in the depletion Region, the electrons move to the left when excited from the valence band to the conduction band, but outside of the depletion region how is there current? There must be current throughout the wire not just in the depletion region. Do the sliding electrons somehow push the other electrons to move? I don't understand how this happens if the electrons outside of the depletion region get excited up from the valence band to the conduction band and just fall back down.

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    Replies
    1. yes, you could say perhaps that they do push the other electrons. or actually there is probably a very very small voltage.

      One might want to start by thinking about current in a wire. Imagine a circuit with just one battery and one resistor in series. What makes the electrons go through the wire that makes that circuit?

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