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Use the photodiode equation (25.17) to compute Iphoto /I0 for a silicon solar cell with Voc = 0.7 V. Write the power as a function of voltage and compute the fill factor, the maximum power I V attainable as a fraction of IphotoVoc. Repeat the calculation for cells with Voc = 0.5 and 0.86 V and compute the maximum efficiency of a single-junction silicon photocell in these cases. give answer in 3step with explanation at the end of each step and final answer at the endI= Into + Io = Liitusion = Iphoto =o (157 — 1) . (25.17)

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Use the photodiode equation (25.17) to compute Iphoto /I0 for a silicon solar cell with Voc = 0.7 V. Write the power as a function of voltage and compute the fill factor, the maximum power I V attainable as a fraction of IphotoVoc. Repeat the calculation for cells with Voc = 0.5 and 0.86 V and compute the maximum efficiency of a single-junction silicon photocell in these cases. give answer in 3step with explanation at the end of each step and final answer at the endUploaded ImageI= Into + Io = Liitusion = Iphoto =o (157 — 1) . (25.17)

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Asked by: amu
Created at: 2025-07-26 20:29:56

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Let's solve the problem step by step, using the photodiode equation provided: \[ I = I_\text{photo} - I_0 \left( e^{eV/k_BT} - 1 \right) \] where: - \( I \) = output current - \( I_\text{photo} \) = photocurrent (generated by sunlight) - \( I_0 \) = dark saturation current - \( V \) = output voltage - \( k_B \) = Boltzmann constant (\( 8.617 \times 10^{-5} \) eV/K) - \( T \) = temperature (assume 300 K for room temperature) - \( e \) = elementary charge (\( 1.602 \times 10^{-19} \) C) We are given: open-circuit voltage \( V_{oc} \) (try for 0.7 V, 0.5 V, and 0.86 V). --- ## **Step 1: Find \( I_\text{photo}/I_0 \) for each \( V_{oc} \)** At open circuit, \( I = 0 \): \[ 0 = I_\text{photo} - I_0 \left( e^{eV_{oc}/k_BT} - 1 \right) \] \[ I_\text{photo} = I_0 \left( e^{eV_{oc}/k_BT} - 1 \right) \] \[ \frac{I_\text{photo}}{I_0} = e^{eV_{oc}/k_BT} - 1 \] Let's calculate for each \( V_{oc} \): Let \( k_BT/e \approx 0.02585 \) V at 300 K. ### a) \( V_{oc} = 0.7 \) V \[ \frac{I_\text{photo}}{I_0} = e^{0.7/0.02585} - 1 \approx e^{27.08} - 1 \approx 5.32 \times 10^{11} \] ### b) \( V_{oc} = 0.5 \) V \[ \frac{I_\text{photo}}{I_0} = e^{0.5/0.02585} - 1 \approx e^{19.33} - 1 \approx 2.48 \times 10^{8} \] ### c) \( V_{oc} = 0.86 \) V \[ \frac{I_\text{photo}}{I_0} = e^{0.86/0.02585} - 1 \approx e^{33.28} - 1 \approx 3.03 \times 10^{14} \] **Explanation:** This ratio is huge because the photocurrent is much larger than the dark current in a well-designed solar cell. --- ## **Step 2: Write Power as a Function of Voltage and Find Maximum Power Point (Fill Factor)** The output power is: \[ P = I V = \left[ I_\text{photo} - I_0 \left( e^{eV/k_BT} - 1 \right) \right] V \] To maximize \( P(V) \), set \( dP/dV = 0 \): \[ \frac{dP}{dV} = 0 = I + V \frac{dI}{dV} \] Let's define \( x = \frac{eV}{k_BT} \), so \( V = x \frac{k_BT}{e} \). \[ I = I_\text{photo} - I_0 ( e^x - 1 ) \] \[ P = I V = [ I_\text{photo} - I_0 (e^x - 1) ] \cdot x \frac{k_BT}{e} \] Set derivative to zero for maximum power: \[ \frac{dP}{dx} = \frac{k_BT}{e} \left[ I_\text{photo} - I_0 (e^x - 1) - I_0 x e^x \right] = 0 \] \[ I_\text{photo} - I_0 (e^x - 1 + x e^x) = 0 \] \[ \frac{I_\text{photo}}{I_0} = e^x (1 + x) - 1 \] Recall from **Step 1** that at \( V_{oc} \), \( \frac{I_\text{photo}}{I_0} = e^{x_{oc}} - 1 \), where \( x_{oc} = \frac{e V_{oc}}{k_B T} \). So, **to find the maximum power point \( x_{mp} \)**, solve: \[ e^{x_{oc}} - 1 = e^{x_{mp}} (1 + x_{mp}) - 1 \] \[ e^{x_{oc}} = e^{x_{mp}} (1 + x_{mp}) \] \[ e^{x_{oc} - x_{mp}} = 1 + x_{mp} \] \[ x_{oc} - x_{mp} = \ln(1 + x_{mp}) \] This equation must be solved numerically for \( x_{mp} \). ### For \( V_{oc} = 0.7 \) V (\( x_{oc} = 27.08 \)) \[ 27.08 - x_{mp} = \ln(1 + x_{mp}) \] Guess \( x_{mp} \approx x_{oc} - \ln x_{oc} \) for large \( x_{oc} \): - \( \ln(27.08) \approx 3.3 \) - \( x_{mp} \approx 27.08 - 3.3 = 23.78 \) - Check: \( \ln(1 + 23.78) \approx 3.2 \), so \( 27.08 - 23.78 = 3.3 \), matches. #### Fill Factor (FF): \[ V_{mp} = x_{mp} \frac{k_BT}{e} \] \[ I_{mp} = I_\text{photo} - I_0 (e^{x_{mp}} - 1) \] \[ I_{mp} = I_0 [ e^{x_{oc}} - 1 - ( e^{x_{mp}} - 1 ) ] = I_0 [ e^{x_{oc}} - e^{x_{mp}} ] \] \[ FF = \frac{V_{mp} I_{mp}}{I_\text{photo} V_{oc}} \] But \( I_\text{photo} V_{oc} = I_0 ( e^{x_{oc}} - 1 ) V_{oc} \). \[ FF = \frac{ x_{mp} \frac{k_B T}{e} \cdot I_0 ( e^{x_{oc}} - e^{x_{mp}} ) }{ I_0 ( e^{x_{oc}} - 1 ) x_{oc} \frac{k_B T}{e} } = \frac{ x_{mp} ( e^{x_{oc}} - e^{x_{mp}} ) }{ x_{oc} ( e^{x_{oc}} - 1 ) } \] Since \( e^{x_{oc}} \gg 1 \), \( e^{x_{oc}} - 1 \approx e^{x_{oc}} \): \[ FF \approx \frac{ x_{mp} ( 1 - e^{x_{mp}-x_{oc}} ) }{ x_{oc} } \] But \( e^{x_{mp}-x_{oc}} = 1/(1 + x_{mp}) \) from earlier. So, \[ FF \approx \frac{ x_{mp} ( 1 - \frac{1}{1 + x_{mp}} ) }{ x_{oc} } = \frac{ x_{mp} \frac{x_{mp}}{1 + x_{mp}} }{ x_{oc} } = \frac{ x_{mp}^2 }{ x_{oc} ( 1 + x_{mp} ) } \] Plug in numbers. - \( x_{oc} = 27.08 \) - \( x_{mp} = 23.78 \) - \( 1 + x_{mp} = 24.78 \) \[ FF = \frac{ (23.78)^2 }{ 27.08 \times 24.78 } \approx \frac{565.5}{671.4} \approx 0.842 \] --- ## **Step 3: Repeat for \( V_{oc} = 0.5 \) V and \( V_{oc} = 0.86 \) V** ### **a) \( V_{oc} = 0.5 \) V** - \( x_{oc} = 0.5 / 0.02585 = 19.33 \) - \( x_{mp} \approx 19.33 - \ln(19.33) \approx 19.33 - 2.96 = 16.37 \) - \( 1 + x_{mp} = 17.37 \) \[ FF = \frac{ (16.37)^2 }{ 19.33 \times 17.37 } \approx \frac{268.1}{336.0} \approx 0.798 \] --- ### **b) \( V_{oc} = 0.86 \) V** - \( x_{oc} = 0.86 / 0.02585 = 33.28 \) - \( x_{mp} \approx 33.28 - \ln(33.28) \approx 33.28 - 3.51 = 29.77 \) - \( 1 + x_{mp} = 30.77 \) \[ FF = \frac{ (29.77)^2 }{ 33.28 \times 30.77 } \approx \frac{886.3}{1024.3} \approx 0.865 \] --- ### **Maximum Efficiency** The maximum *fraction* of \( I_\text{photo} V_{oc} \) attainable is the fill factor (\( FF \)), so: - For \( V_{oc} = 0.7 \) V: \( FF \approx 0.84 \) - For \( V_{oc} = 0.5 \) V: \( FF \approx 0.80 \) - For \( V_{oc} = 0.86 \) V: \( FF \approx 0.87 \) --- ## **Summary Table** | \( V_{oc} \) (V) | \( I_\text{photo}/I_0 \) | Fill Factor (FF) | Max Power as Fraction of \( I_\text{photo} V_{oc} \) | |:---------:|:----------------------:|:----------------:|:----------------------------------------------------:| | 0.5 | \( 2.5 \times 10^8 \) | 0.80 | 0.80 | | 0.7 | \( 5.3 \times 10^{11} \) | 0.84 | 0.84 | | 0.86 | \( 3.0 \times 10^{14} \) | 0.87 | 0.87 | --- ## **Final Answer** > **Step 1:** Calculated \( I_\text{photo}/I_0 \) for each \( V_{oc} \), using the photodiode equation at open circuit. > > **Step 2:** Derived the power-voltage relationship, found the fill factor (FF) and maximum output power as a fraction of \( I_\text{photo} V_{oc} \). > > **Step 3:** Repeated for other \( V_{oc} \) values and summarized results. > > **So, for a silicon solar cell:** > - At \( V_{oc} = 0.7 \) V, \( I_\text{photo}/I_0 \approx 5.3 \times 10^{11} \), FF ≈ 0.84. > - At \( V_{oc} = 0.5 \) V, \( I_\text{photo}/I_0 \approx 2.5 \times 10^8 \), FF ≈ 0.80. > - At \( V_{oc} = 0.86 \) V, \( I_\text{photo}/I_0 \approx 3.0 \times 10^{14} \), FF ≈ 0.87. > > **The maximum power attainable is about 80–87% of \( I_\text{photo} V_{oc} \) depending on \( V_{oc} \).**

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