4.8.4 · D1Spectroscopy & Analysis (Intro)

Foundations — ¹H NMR — chemical shift, multiplicity (n + 1 rule), integration; common ranges

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Before you can read the parent note (¹H NMR topic), you need every symbol it throws at you built from nothing. We go in dependency order: each idea below is used by the next.


0. What is a proton here, really?

Why the topic needs it: the entire method exists only because this tiny magnet can be pushed around by a big magnet. No magnetic proton, no NMR.


1. The external field

Why the topic needs it: the two allowed orientations are two energy levels. The whole experiment is about the gap between them.


2. Energy levels and the energy gap

Why the topic needs it: "which radio note does this proton absorb" is "how big is its gap," which is "how strong a field does it locally feel."


3. Frequency — the radio note

Why the topic needs it: this single line links the measurable thing (frequency) to the hidden thing (local field). Everything else decodes the local field.


4. The gyromagnetic ratio

Why the topic needs it: is a constant, so it will cancel later when we build — but you must know it's there to see it cancel.


5. Shielding constant and the local field

Why the topic needs it: chemical shift is entirely a story about . Different chemical environments = different electron umbrellas = different = different notes. This is why NMR can tell environments apart. (Electron pulling is governed by Electronegativity and, for rings, by Aromaticity & ring current.)


6. Reference, and why we need TMS

Why the topic needs it: without a shared zero, no two spectra could be compared. TMS is that shared zero.


7. Parts per million (ppm) and the symbol


8. Integration — area, not height

Why the topic needs it: chemical shift tells you what kind of proton; integration tells you how many of that kind — the second of the three readings.


9. Neighbours, "vicinal", and equivalence

Why the topic needs it: the splitting rule counts vicinal, non-equivalent neighbours only. Miscounting here is the #1 error.


10. Spin states, ↑ and ↓, and coupling

Why the topic needs it: this is the mechanism behind the rule and its intensity pattern.


11. Counting combinations: , , and

Why the topic needs it: it turns "count spin combinations" into a clean formula, delivering both the number of lines () and their heights (Pascal row).


12. The rule, assembled

Every symbol in that sentence is now earned: = count of vicinal non-equivalent neighbours (§9), the lines come from their spin states (§10), and the heights come from (§11).


Prerequisite map

proton is a tiny magnet

external field B0 two energy levels

energy gap delta E

radio frequency nu

gyromagnetic ratio gamma

electrons shield sigma

local field B0 times one minus sigma

TMS reference zero

chemical shift delta in ppm

area equals proton count

integration reading

vicinal and equivalent neighbours

spin states up and down

binomial choose n k

Pascal triangle intensities

n plus 1 rule

read a 1H NMR spectrum


Equipment checklist

Cover the right side and test yourself.

A proton in NMR is
a hydrogen nucleus behaving as a tiny bar magnet
is
the strong steady external magnetic field the sample sits in
Why are there two energy levels?
the proton-magnet can align with or against
(nu) is
the frequency of the radio wave that flips the proton
(gamma) is
a fixed constant per nucleus type; it cancels when forming
(sigma) is
the shielding constant — how much electrons screen the proton
Why do we use TMS?
it sets a shared zero so labs can compare spectra
Why divide by spectrometer frequency in ?
it cancels , making field-independent
Why ×10⁶ in ?
the raw ratio is tiny; scaling gives convenient ppm numbers
Integration measures
the area under a peak = number of protons (as a ratio)
Vicinal protons are
protons on the adjacent carbon (three bonds away)
Do equivalent protons split each other?
no
equals
, the count of ways to choose from
Row of Pascal's triangle sums to
The rule says
equivalent vicinal neighbours give lines