Intuition The ONE core idea
A hydrogen atom is like a ball resting on one of several fixed steps of a staircase; when the ball drops to a lower step it spits out a flash of light whose colour is set entirely by how far it fell . Because the step heights are fixed, hydrogen always glows the same set of colours — and this page builds, one symbol at a time, every piece of vocabulary you need to read that story.
Before you can trust the parent note , you need every symbol it throws at you to already mean something. Below, each symbol is introduced only after the one it depends on. Read top to bottom — nothing is used before it is built.
Intuition How the figures are numbered
This page has three figures, labelled Figure 1 (s01) , Figure 2 (s02) , Figure 3 (s03) . Each one appears right after the section that needs it, and the text always names it explicitly. When you read "Figure 1", scroll to the picture tagged s01.
Definition The electron and its orbit
An electron is the tiny negatively-charged particle that circles the centre of the atom. In the picture, it is the small dot moving on a ring around the heavy central nucleus (the positive core). The ring it sits on is called an orbit — think "which floor of a building the electron lives on".
Figure 1 (s01) — the rings of the atom.
Why do we need this picture at all? Because the whole topic is about the electron changing which ring it lives on . If you cannot see the rings, the rest is just symbols. Everything about these rings comes from the Bohr Model of the Atom .
n — the principal quantum number
n is just a counting label for the rings: n = 1 is the innermost ring (closest to the nucleus), n = 2 the next one out, n = 3 after that, and so on. It is always a whole number: n = 1 , 2 , 3 , … — never 1.5 , never 0 .
Picture: number the rings from the inside out. n = "which ring".
Why a whole number and not any number? Because the electron is not allowed to sit between rings — a rule called quantization (see Quantization of Angular Momentum ). This "only whole steps allowed" fact is the reason hydrogen produces sharp, separate colours instead of a smear.
Intuition Why the steps get squished at the top
Look at Figure 1 (s01) : the low rings are far apart, the high rings crowd together. So a jump near the bottom covers a big energy drop, and a jump near the top covers a tiny one. Hold onto this — it explains every wavelength ordering later.
E and the level energy E n
Energy is "how much oomph" something has — here, how strongly the electron is bound to the nucleus. E n means "the energy of the electron when it sits on ring number n ". The little n underneath is a subscript : it just says which ring this energy belongs to. E 2 = energy on ring 2.
Picture: height of each step on an energy staircase.
Definition The unit "eV" (electron-volt)
Energies this small are measured in electron-volts , written eV . One eV is a fixed tiny packet of energy — you don't need its exact value, just treat "eV " like "metre" or "second": a unit that comes along for the ride. See Photon Energy and Planck's Relation .
Common mistake "Higher floor = more energy, so
E n is bigger there"
Why it feels right: climbing stairs does take more effort, so higher should mean bigger number.
The trap: the numbers are negative . From the rule, E 1 = − 13.6 eV and E 2 = − 3.4 eV . Since − 3.4 is greater than − 13.6 , the higher floor really does have more energy — but the number looks smaller because it's less negative.
Fix: read it like temperature below zero: − 3 ∘ is warmer than − 1 3 ∘ . The minus sign means "bound"; E = 0 is the free electron at the top of the staircase.
A photon is one single particle-packet of light. When the electron drops a floor, exactly one photon is born, carrying away the energy that was lost.
Picture: a wavy arrow leaving the atom — exactly the squiggle whose shape we zoom into in Figure 2 (s02) right below.
λ (the Greek letter "lambda")
λ is the length of one wave of that photon — the distance from one crest to the next. Short λ = high-energy light (blue/UV); long λ = long-wavelength light (red/infrared).
Picture: the gap between two crests of the squiggle.
Figure 2 (s02) — what a wavelength is.
Why do we care about λ and not just energy? Because λ is what a spectrometer actually measures — it is the observable colour. Energy is the cause; λ is the visible effect.
c , ν , h (with their values)
c is the speed of light — a fixed constant, c ≈ 3.00 × 1 0 8 m/s : how fast the photon travels.
ν (Greek "nu", looks like an italic v) is the frequency : how many wave-crests pass per second, in s − 1 .
h is Planck's constant , h ≈ 6.63 × 1 0 − 34 J⋅s (= 4.14 × 1 0 − 15 eV⋅s ): the fixed conversion factor that turns "frequency" into "energy".
Why the tool "h c / λ " and not something else? We have a wavelength (what we see) but want an energy (what caused it). This one equation is the exact bridge between the two — it is the whole reason a fixed energy drop gives a fixed colour. This is the heart of Photon Energy and Planck's Relation .
Mnemonic The 1240 shortcut
Multiply the two constants: h c = ( 4.14 × 1 0 − 15 eV⋅s ) ( 3.00 × 1 0 8 m/s ) ≈ 1.24 × 1 0 − 6 eV⋅m = 1240 eV⋅nm . So λ ( nm ) = E ( eV ) 1240 . Energy in eV in, wavelength in nm out.
Before we combine anything, meet the triangle symbol. Δ (Greek capital delta, drawn as a triangle) is the mathematician's shorthand for "change in" or "difference of" . So Δ E literally reads "the difference of two energies" — nothing more. Only once you know that can the header of this section, and the equation below, make sense.
Δ E (the symbol "delta E")
Now that Δ means "difference of", we want Δ E to come out positive — it is the size of the drop , the energy handed to the photon — so on this page we deliberately write "higher minus lower":
Δ E = E n 2 − E n 1 ( n 2 > n 1 )
Because E n 2 (higher floor, less negative) is greater than E n 1 (lower floor, more negative), this difference is a positive number.
Why not the textbook "final minus initial" order? In many books Δ E = E final − E initial , which for a fall is negative (energy lost). That is fine for bookkeeping, but here we only care about the magnitude of light emitted, so we choose the order that makes Δ E positive and matches the parent note's Rydberg form n 1 2 1 − n 2 2 1 . Same physics, sign chosen for clarity.
Picture: the vertical height of the arrow from the start floor to the landing floor in Figure 3 (s03).
Figure 3 (s03) — a fall from n 2 to n 1 emits a photon.
Why keep two separate labels? Because the landing floor n 1 names the whole family (the series), while the starting floor n 2 picks which single line within that family. Getting them backwards is the number-one mistake — the parent note devotes a whole warning to it.
1/ λ
λ 1 is one divided by the wavelength — literally "how many waves fit in one metre". Big 1/ λ = many short waves = high energy. It has units m − 1 (per metre).
Why bother flipping it? Because energy is proportional to 1/ λ , not to λ . Working in 1/ λ keeps the master formula a clean straight-line relationship instead of a messy reciprocal.
Definition The Rydberg constant
R H
R H is a single fixed number, R H ≈ 1.097 × 1 0 7 m − 1 , that bundles together all the physical constants (13.6 eV , h , c ). The subscript H reminds us it is the value for Hydrogen — one electron only.
Z — the nuclear charge (atomic number)
Z is the number of protons in the nucleus , also called the atomic number . Hydrogen has Z = 1 (one proton). A helium ion He + that has lost one electron still has Z = 2 (two protons) but only one electron left — a hydrogen-like ion . A bigger Z pulls the lone electron in harder, deepening every energy level. For such one-electron ions you multiply the wavenumber by Z 2 :
λ 1 = R H Z 2 ( n 1 2 1 − n 2 2 1 )
That Z 2 factor is the whole point of Hydrogen-like Ions and Z dependence . For plain hydrogen Z = 1 , so Z 2 = 1 and the factor quietly disappears.
With every symbol now built, the parent's master equation reads in plain words:
waves per metre λ 1 = fixed number R H landing floor n 1 2 1 − start floor n 2 2 1
If the electron gets enough energy to climb all the way past the top of the staircase, it leaves the atom entirely — the atom is ionized . This happens as n → ∞ , where E n → 0 . The energy needed to do this from the ground floor is the ionization energy , 13.6 eV (see Ionization Energy ).
Picture: the dashed "escape line" at the top of Figure 1 (s01).
n 2 → ∞ (the arrow "to infinity")
→ ∞ means "let the starting floor get bigger and bigger without end". Then 1/ n 2 2 → 0 and the formula loses its second term. This gives the series limit — the shortest wavelength of a series, from an electron falling in from the very edge of freedom.
Energy level E_n equals minus 13.6 over n squared
Photon and wavelength lambda
Photon energy hc over lambda
Photon energy equals delta E
Wavenumber and Rydberg R_H
Ionization and series limit
Charge Z scaling for ions
Read it as: orbits give the floor number n , which sets each energy E n ; differences of those energies drive a photon whose energy equals that drop; converting that energy to a wavelength and grouping by landing floor produces the named series, with Z scaling it up for heavier one-electron ions.
Cover the right side and test yourself. If any answer surprises you, re-read that section before the parent note.
What does the subscript in E n mean "which ring/floor", n = 1 , 2 , 3 , …
State the rule for E n E n = − 13.6 eV / n 2
Why is E n negative the electron is bound; E = 0 is the free electron at the top
Which is greater, E 1 = − 13.6 or E 2 = − 3.4 E 2 (less negative = higher energy)
What is a photon one single packet of light emitted when the electron drops
What does λ measure the length of one wave; short = high energy, long = low energy
What does Δ (delta) mean "change in" / "difference of"
On this page, what is Δ E E n 2 − E n 1 , chosen positive = size of the drop
What links the photon to the drop E photon = Δ E
In a fall, which floor is n 1 and which is n 2 n 1 = lower landing floor, n 2 = higher start floor
Which equation links wavelength to energy E = h c / λ
Values of c and h c ≈ 3.00 × 1 0 8 m/s , h ≈ 6.63 × 1 0 − 34 J⋅s
Fast eV-to-nm shortcut λ ( nm ) = 1240/ E ( eV )
Why work in 1/ λ not λ energy is proportional to 1/ λ , keeping the formula linear
What is R H and its value Rydberg constant for hydrogen, 1.097 × 1 0 7 m − 1
What is Z number of protons in the nucleus (atomic number); Z = 1 for hydrogen
How does the formula change for a one-electron ion multiply by Z 2
What does n 2 → ∞ physically mean electron falls in from the ionization edge → series limit
What is ionization electron escapes the atom entirely; E n → 0 as n → ∞
Bohr Model of the Atom — where the quantized rings and E n = − 13.6/ n 2 come from.
Quantization of Angular Momentum — why n must be a whole number.
Photon Energy and Planck's Relation — the E = h c / λ bridge built in §5.
Ionization Energy — the top of the staircase and the series limit.
Hydrogen-like Ions and Z dependence — how R H generalizes with Z 2 .
Emission vs Absorption Spectra — falls emit, climbs absorb; same floors, opposite arrows.