1.8.1 · D2Electromagnetism

Visual walkthrough — Electric charge — properties, quantization, conservation

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We build one idea per step. Follow the figures in order; the pink, yellow and blue chalk strokes carry the argument.


Step 1 — Start with a single indivisible brick

WHAT. Nature does not hand us charge in a smooth stream. It hands us tiny identical carriers. The smallest free carrier of charge is the electron, and the amount of charge it carries has a fixed magnitude we call (the elementary charge).

WHY start here. Before we can count anything we need one thing to count — a unit that never splits. If the unit could be halved, "how many" would be meaningless. So we first fix the brick.

PICTURE. A single chalk circle = one electron. Beside it we write its charge value.

Figure — Electric charge — properties, quantization, conservation

The number just says the brick is extremely small compared to a coulomb — hold that thought, it explains Step 8.


Step 2 — Charge has a colour: the two signs

WHAT. A brick can carry its charge in one of exactly two "flavours": positive () or negative (). An electron's brick is negative; a proton's brick is positive, but the magnitude is identical.

WHY two, not one. Two simple experiments force the issue. (1) Rub a glass rod with silk and hang it up; bring a second rubbed glass rod near it — they push apart. (2) Rub a plastic rod with fur and bring it near the hanging glass rod — they pull together. Same-treatment rods repel; opposite-treatment rods attract. A single flavour could only ever do one of those behaviours. Two flavours — with a sign to tell them apart — is the minimum needed to explain both.

PICTURE. The two experiments drawn side by side (glass–glass repel, glass–plastic attract), then the two bricks they justify: one pink with a , one yellow with a . Same size (same ), opposite label.

Figure — Electric charge — properties, quantization, conservation

Step 3 — Stacking identical bricks: repeated addition

WHAT. We now name the charge on a whole object. Let stand for that object's total charge, and let (read "the size of ") mean its magnitude — the amount ignoring the label. Suppose the object has extra electrons, all identical. Then its charge magnitude is the size of one brick added to itself times.

WHY addition. Each brick contributes the same amount , independently. When identical things pile up and each adds the same fixed amount, "add , times" is exactly what multiplication means. That is the whole reason a appears.

PICTURE. A stack of pink bricks; a bracket labels the pile " bricks", and the running total climbs

Figure — Electric charge — properties, quantization, conservation

Reading it term by term:

  • — the total charge magnitude on the object (the height of the whole stack).
  • each — one brick's contribution.
  • — how many bricks we stacked (a plain whole number: ).
  • — the shortcut for " added times."

This is the quantization of charge: allowed charges are only , never anything in between, because you cannot stack half a brick.


Step 4 — Invert the stack: the counting formula

WHAT. Usually we measure the total charge magnitude and want to know how many bricks made it. So we run Step 3 backwards.

WHY divide. If bricks of size give total , then asking "how many bricks?" means "how many times does one brick fit inside the total ?" — and "how many times does one thing fit inside another" is precisely division.

PICTURE. The same stack, now with a chalk ruler of length laid against it, ticking off how many brick-heights fit into .

Figure — Electric charge — properties, quantization, conservation

The units cancel — coulomb over coulomb — leaving a bare count, exactly as a "how many" answer should be.


Step 5 — Use it: a worked count

WHAT. A body carries . How many electrons were added?

WHY. This is Step 4 with numbers. The minus sign tells us the flavour (extra negative bricks = electrons gained); the magnitude tells us how many.

PICTURE. The ratio drawn as "big bag tiny brick," with the answer written on the board.

Figure — Electric charge — properties, quantization, conservation

Step 6 — The signed total: additivity across a box

WHAT. Put several charged objects in one box. The box's total charge is the sum — but with signs, because pink () bricks cancel yellow () bricks one-for-one.

WHY signed sum, not plain sum. A brick and a brick together push and pull on the outside world by equal and opposite amounts — they neutralise. So they must add to zero, not to . Only a signed sum does that.

PICTURE. A box holding some yellow and some pink bricks; pairs annihilate visually, leaving a small net pile whose colour is the leftover flavour.

Figure — Electric charge — properties, quantization, conservation
  • — each object's own signed charge (yellow , pink ).
  • — "add them all up, keeping signs."
  • — the single signed number describing the whole box.

Step 7 — The sealed box never changes: conservation

WHAT. If the box is isolated (nothing charged crosses its wall), then no matter how the bricks rearrange inside, the signed total stays fixed as time passes.

WHY. Bricks can move between objects and pairs can be created or destroyed together, but a brick never appears or vanishes alone. Every event changes the count by . So the running total cannot budge.

PICTURE. Two panels of the same box, "before" and "after" an internal shuffle: the arrangement differs, the tally at the bottom is identical.

Figure — Electric charge — properties, quantization, conservation

Before writing this in symbols, let = time (a clock reading, measured in seconds). We want to say " does not change as the clock advances." The compact way to write "the rate at which a quantity changes as time advances" is the derivative, written — read it literally as "how fast changes per second." If a quantity holds perfectly steady, that rate is exactly . So "the total is frozen in time" becomes:

  • — the time (clock reading, in seconds).
  • — the rate at which the total changes per second.
  • — that rate is zero, i.e. it does not change at all.
  • The arrow: therefore the tally before equals the tally after.

Step 8 — The edge and degenerate cases (never leave the reader stranded)

Every scenario must be covered. Here are the boundary cases the formula must survive.

Case A — the neutral object, . Equal numbers of yellow and pink bricks. . Not "no charge exists," but "charges cancel." Perfectly allowed ( is a whole number).

Case B — a fractional answer is forbidden. Ask: can a free body carry ? is not a whole number ⇒ impossible. You cannot stack half a brick. The formula's integer-ness is a physical veto.

Case C — why the steps look invisible in daily life. One coulomb is The step from to is one part in — like adding one grain to a beach. So charge looks smooth even though it is grainy.

Case D — the "smaller brick" trap (quarks). Quarks carry , seemingly a smaller brick. But quarks are confined — never free. Any observable free charge is still a whole multiple of .

PICTURE. Four mini-panels: (A) balanced box ; (B) a -brick stack with a red cross; (C) a beach of dots to show smoothness; (D) three thirds locked inside one particle.

Figure — Electric charge — properties, quantization, conservation

The one-picture summary

Figure — Electric charge — properties, quantization, conservation

One brick → stack of them → total → invert to count → sum with signs across a box → and the sealed box's tally never moves. That single chain is all three properties at once: Quantized (whole bricks), Additive (signed sum), Conserved (fixed tally).

Recall Feynman retelling — the whole walkthrough in plain words

Charge comes in identical little bricks, each the same size , and each painted one of two colours: yellow for plus, pink for minus. If you pile up pink bricks you get charge — that's just adding the same brick over and over, which is multiplying. Turn that around and you can count the bricks in any charge by dividing the total by one brick: . When you divide and don't get a whole number, you've described a pile that can't exist, because half a brick isn't a thing. Throw a bunch of objects into a sealed box and the box's charge is the bricks added up with their colours — a yellow and a pink cancel to nothing. And here's the magic: shake the box, let bricks jump between objects, even let plus-minus pairs appear and vanish — the tally at the bottom of the box never changes, because bricks are always born and die in matched pairs. Whole bricks, signed sums, frozen tally: quantized, additive, conserved.


Active recall

Why must in be a whole number?
Charge is built from indivisible identical bricks ; you cannot stack a fraction of a brick.
Where does the division in come from?
"How many bricks of size fit in the total " is division by definition.
Why do charges add with signs (not plain magnitudes)?
A and a neutralise each other, so they must sum to , which only a signed sum gives.
In a sealed box, why is the total charge frozen?
Bricks only move or are created/destroyed in pairs, each event changing the tally by .
Two identical spheres and touch — final charge each?
Total is fixed; equal geometry splits it, giving each.
Why does grainy charge look smooth in everyday life?
One coulomb is about bricks, so the step from to is negligibly small.