NMR: Theory and Equivalence. Nuclear Magnetic Resonance Powerful analysis – Identity – Purity No authentic needed Analyze nuclei – 1 H, 13 C, 31 P, etc.

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Presentation transcript:

NMR: Theory and Equivalence

Nuclear Magnetic Resonance Powerful analysis – Identity – Purity No authentic needed Analyze nuclei – 1 H, 13 C, 31 P, etc – Get information of how they are attached

Nuclear Magnetic Resonance Nuclear – Based on nuclear spin Magnetic – Large electromagnets create energy differences in nuclei Resonance – Signal based on absorbed light in resonance with energy difference

Nuclear Spin Some nuclei have spin – 1 H, 13 C No spin if nuclei have even number of protons and neutrons ( 12 C) Nuclei align spin with and against magnetic field

External Magnetic Field Bigger energy difference between spin states For absorption, E photon = E spin gap Spin flip occurs Consider the proton NMR spectrum of CH 4

NMR Spectrum CH 4 in magnet Protons line up with/against RF energy Only RF energy = gap energy absorbed Spectrum shows an absorption

Magnetic Field Experienced Not all nuclei in a molecule experience the same magnetic field, even if they are in the same magnet Why? Shielding! Consider CH 3 Cl

NMR Spectrum CH 3 Cl in magnet Electronegative Cl deshield protons Protons experience bigger external field Only RF energy = gap energy absorbed Spectrum shows a higher frequency absorption

NMR Spectrum Need standard: TMS (shielded) Need relative frequency: ppm ppm = Hz shift/ MHz magnet 60 mHz 200 MHz

Other Sources of Shielding Anisotropy Different effect along different axis Can have dramatic shielding/ deshielding effects

Four Questions How many signals? Equivalence Where on spectrum? Chemical Shift How big? Integration Shape? Splitting (coupling)

Number of Signals Four sets of protons in different chemical environments Four sets of equivalent protons Leads to four distinct signals

Equivalence Experience same average magnetic field due to – Free rotation – Plane of symmetry – Axis of symmetry

How many 13 C signals?

How many 1 H signals?

A more complicated problem