Electricity/5 min exploration

How does a solar panel work? Cells, strings and shade

A solar panel turns light into electricity in silicon cells.

Light frees charge carriers at each cell's p–n junction, and the junction separates them so an external circuit can deliver current. Series-connected cells add their voltages but must share one current, which is why one shaded cell can restrict its whole string. A bypass diode provides an alternate path around a reverse-biased string so the remaining strings can keep supplying power.

How does sunlight become electricity, and why can one shaded cell hold back a whole string?

3D model

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Model view

What to remember

Each cell converts light to current and series cells add voltage, but a shaded cell can limit its whole string; a bypass path lets the other strings keep delivering power instead of forcing all current through the shaded cell.

With cell A01 fully shaded and the bypass conducting, the panel delivers 104.3 W. Predict what happens when you disable the bypass diodes, keeping sunlight, tilt and the 5 Ω load unchanged.

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How the parts work together

  1. Light becomes an electric current

    Face the panel directly into full sunlight. The 60 cells deliver 216.2 W to the fixed 5 Ω load in this ideal model: 32.88 V and 6.58 A. Reduce sunlight or tilt the panel and the incident light, current and power fall. The moving amber marks are a light cue, not a photon-rate calculation.

  2. Series cells add voltage but share current

    Open the layer stack. Glass and encapsulant protect the cells; the rear layers insulate them. The magnified p–n inset names the two doped silicon regions. The panel has three strings of 20 series cells: within each string, every cell carries the same current while their voltages add.

  3. A bypass protects the working strings

    Cell A01 is now fully shaded. With its ideal bypass conducting, string A contributes 0 V and the other two strings deliver 104.3 W to the same load. Switch the bypass diodes off: this ideal circuit has no valid forward operating point and output becomes 0 W. Real modules have losses and reverse-behavior that this comparison deliberately omits.

The main parts

60 silicon cells
Sixty clipped-corner silicon wafers in three 20-cell series strings. Cell A01 is the one covered by the shade control.
Glass & front encapsulant
A transparent front sheet and encapsulant protect the cells while admitting light. Their thicknesses are enlarged for the layer view.
Rear encapsulant & backsheet
Rear layers support and insulate the cell laminate. The model does not calculate weathering or insulation strength.
Aluminium frame
Four joined rails surround the laminate and give the panel a recognizable rigid edge.
Cell busbars & string interconnects
Two silver busbars on each cell represent the conductive collection paths. The circuit card makes the three series strings explicit.
Rear junction box
A protective box on the back joins the strings to the output cable and houses the three illustrated bypass paths.
Three ideal bypass diodes
One ideal diode is connected across each 20-cell string. In this model it clamps a reverse-biased string at 0 V; real diode loss and heat are omitted.
p-type silicon
Boron-doped silicon has electron vacancies called holes. In the magnified inset it forms the base side of the teaching junction.
n-type silicon
Phosphorus-doped silicon contributes free electrons and forms the light-facing emitter in this teaching junction. The inset is symbolic and greatly magnified, not a thickness-scale fabrication drawing.

Questions worth exploring

How does a solar cell make electricity?

A silicon cell contains p-type and n-type regions. Light frees charge carriers and the p–n junction separates them, allowing current to flow through an external circuit. The panel converts light directly to electrical energy; it does not need a spinning generator. The magnified junction in this lesson is a symbolic teaching view, not a fabrication-scale drawing.

U.S. DOE · PV Cells 101: A Primer on the Solar Photovoltaic Cell (semiconductor conversion, contacts and modules)OpenStax · University Physics Volume 3 · 9.6 Semiconductors and doping

Why can one shaded cell reduce a solar panel's output?

Cells in a series string carry the same current. A shaded cell produces less photocurrent, so it can limit every healthy cell in that string even though they remain lit. In this ideal fixed-load model, a fully shaded cell blocks the string completely when no bypass or reverse-breakdown path is available.

NREL · Characterizing Shading Losses on Partially Shaded PV Systems (15–20-cell substrings and series current)

What does a bypass diode do in a solar panel?

In this lesson's ideal circuit, a bypass diode turns on when its 20-cell string becomes reverse-biased. It gives panel current a route around that string, so the other two strings can keep delivering power. The model clamps the bypassed string to 0 V and omits real diode voltage loss, heating and reverse breakdown, so it is not a hot-spot or reliability simulation.

NREL · Characterizing Shading Losses on Partially Shaded PV Systems (15–20-cell substrings and series current)

Why does solar-panel tilt matter?

Tilting a flat panel away from the incoming rays reduces the area it presents to them. This model uses direct irradiance proportional to the cosine of the tilt angle: 60° gives half the face-on value. It omits diffuse sky light and reflections, so it is a geometric demonstration rather than an energy-yield forecast.

U.S. DOE · Tribal Energy Webinar: Solar & Wind (plane-of-array direct-beam cosine)

One discovery leads to another.

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