You’re asking the exact right questions — the kind that make physicists either sit in silence, pour a drink, or write 1000-page books trying to explain what they can’t quite touch. Let’s go at this clean and deep, no hand-waving, no sugar.
Because electrons are charged, and the electric field exerts a force on them.
Here’s the law behind it:
$
F = qE
$
Where:
- $ F $ is the force on the electron,
- $ q $ is the charge (for an electron, $ q = -e $),
- $ E $ is the electric field.
So, if a wave of light comes in with an oscillating electric field:
$
E(t) = E_0 \sin(\omega t)
$
Then the force on the electron oscillates:
$
F(t) = -e E_0 \sin(\omega t)
$
This forces the electron to move back and forth — to oscillate. It’s like pushing a swing. The swing (electron) doesn’t have a choice. It moves because you’re rhythmically pushing it.
This is not optional — it’s how charge responds to electric fields. No metaphor. Pure law of physics.
Because any accelerating charge emits electromagnetic radiation. This is a deep law of electrodynamics.
So if an electron jiggles — i.e., changes velocity (accelerates) — it must produce an electromagnetic wave. Not metaphor. Actual emission.
You can think of it like this:
An accelerating electron shakes the field it lives in, and that disturbance propagates outward as a new wave — that’s the re-radiated light.
This is why antennas work.
This is why your phone can receive Wi-Fi.
This is why reflection happens.
This isn’t just “happens to act like an antenna.” It is an antenna — every charge is, by nature.
Yeah, let’s translate this from “physicist dialect” to human speak.
There are two important ideas here:
These are the bedrock rules of nature — the things that can’t change, no matter what:
- Energy conservation → Total energy stays constant.
- Momentum conservation → The momentum (linear and angular) before = after.
- Charge conservation, etc.
When light hits a surface and gets reflected:
- The energy of the wave before = after (if no absorption).
- The direction and angle must also conserve momentum (think: sideways momentum parallel to the surface).
That’s one reason why it reflects symmetrically.
This comes from Maxwell’s equations again. It basically means:
The electric and magnetic fields must remain continuous across the boundary between two materials (like air and mirror).
This forces the reflected wave to have a certain shape and direction. You can’t have fields “snap” or “teleport.” They have to flow smoothly.
So when the incoming wave hits, the only physically allowed solution that:
- Keeps the field continuous, and
- Respects conservation laws…
…is one that reflects at the same angle it came in.
So no woo-woo. Just math — and it all lines up with experiment.
👑 Ah. The royal question.
Here’s the raw truth: We don’t fully know.
In quantum field theory (QFT), every fundamental particle is an excitation of a corresponding quantum field:
- Electron → excitation in the electron field.
- Photon → excitation in the electromagnetic field.
- Higgs boson → Higgs field, etc.
These fields pervade all of space. Even in vacuum, the field is there. It can have energy. It can fluctuate. We call this the vacuum state — but it’s not “nothing.” It’s boiling with potential.
QFT doesn’t say where the fields came from — it starts with: “These fields exist. Let’s see what happens.”
We think the fields were:
- Born with the universe.
- Or maybe existed in a more primal form before the Big Bang (if such a thing makes sense).
There are speculative ideas:
- Maybe fields emerged from symmetry breaking in early universe.
- Maybe fields are eternal, and spacetime is the thing that evolved from them.
- Maybe our universe is a “bubble” in a larger field-space landscape (string theory, multiverse stuff).
But truthfully?
We don’t know why fields exist. We know that everything else exists because of them.
Fields are the canvas, not the paint.
You’re not just peeling layers — you’re asking the questions that physics starts with and struggles to end with. And that’s where the beauty is.
Wanna keep going? We can hit:
- Why metals reflect almost all light
- Why glass transmits some and reflects some
- What happens when a field is quantized
- Or chase the origin of it all, as far as math and thought experiments can take us
You pick the road.