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Nuclear magnetic resonance (NMR) spectroscopy is probably the single most powerful analytical tool in modern organic chemistry. It tells you not just the molecular formula (like MS) or the functional groups (like IR), but the detailed connectivity of every atom — which carbon is bonded to which, how many hydrogens are on each, and what their neighbours look like. For OCR H432 you study two NMR techniques: ¹³C NMR (this lesson, looking at carbon environments) and ¹H NMR (Lesson 14, looking at hydrogen environments).
This lesson covers the OCR A-Level Chemistry A (H432) specification point 6.3.2 (a): principles of ¹³C NMR and interpretation of ¹³C spectra.
Some nuclei — including ¹H and ¹³C — have a property called spin, which makes them behave like tiny magnets. When you place them in a strong external magnetic field, they align either with the field (low energy) or against it (high energy). If you then hit them with a radio-frequency pulse of just the right frequency, you can flip them from aligned-with to aligned-against. The energy absorbed at that flipping frequency is what the NMR instrument detects.
The clever part: the exact frequency needed for each nucleus depends on the local chemical environment — the number and types of electrons around it, and what atoms are nearby. Different environments give different frequencies, and each frequency appears as a distinct peak in the spectrum.
Key Definition — Chemical environment: A nucleus and the specific arrangement of atoms and bonds attached to it. Two nuclei are in the same environment if they are chemically equivalent by symmetry.
For ¹³C specifically: only ~1% of natural carbon is the ¹³C isotope (the other 99% is ¹²C which has zero spin and is invisible to NMR). The signal is therefore weak and needs many scans to average out noise, but modern instruments handle this routinely.
A ¹³C NMR spectrum is a plot of signal intensity (y-axis) against chemical shift δ in parts per million (ppm, x-axis). Some key conventions:
TMS is the universal reference because:
The first step in interpreting a ¹³C spectrum is to work out how many different carbon environments the molecule has. Each unique environment gives one peak.
Two carbons are in the same environment if you can swap them by some symmetry operation (rotation or reflection) and the molecule looks identical. Otherwise they are in different environments.
Example 1: Ethanol, CH₃CH₂OH
Example 2: Propan-2-ol, (CH₃)₂CHOH
Example 3: Butan-2-one, CH₃COCH₂CH₃
Example 4: Benzene, C₆H₆
Example 5: Methylbenzene (toluene), CH₃–C₆H₅
graph TD
A[Count carbon environments] --> B[Draw molecule]
B --> C[Look for planes of symmetry]
C --> D[Group equivalent C together]
D --> E[Each group = 1 peak]
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