By Alan J. Benesi

ISBN-10: 1118588991

ISBN-13: 9781118588994

Provides the idea of NMR improved with Mathematica© notebooks

- Provides brief, targeted chapters with short reasons of well-defined themes with an emphasis on a mathematical description
- Presents crucial effects from quantum mechanics concisely and for simple use in predicting and simulating the result of NMR experiments
- Includes
*Mathematica*notebooks that enforce the idea within the kind of textual content, photos, sound, and calculations - Based on type established equipment built by means of the writer over his 25 yr educating occupation. those notebooks exhibit precisely how the speculation works and supply worthwhile calculation templates for NMR researchers

**Read Online or Download A Primer of NMR Theory with Calculations in Mathematica PDF**

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**Extra resources for A Primer of NMR Theory with Calculations in Mathematica**

**Sample text**

Ĥ J has a non‐ zero isotropic component. It is used not only for its information content but also for coherence transfer between nuclei. It arises from the indirect coupling of nuclear spins mediated by electron density in orbitals between them. In liquids, Ĥ J_liquid ≠ 0. ˆ H ˆ ˆ ˆ ˆ ˆ H H H H Summarizing, in rigid solids, H Z ˆ H CS Q RF SR D K ˆ . However, due to differences in the electronic environment there is varH J iation in the relative magnitudes, so this order does not always apply.

Energy level). In general, there are a number of n quantized energy levels En and n different eigenfunctions ψn that satisfy this equation. The eigenfunctions ψn are the stationary states of the system. 2) In NMR, the dominant Hamiltonian is the Zeeman Hamiltonian HZ = −γ ħ B0 Îz = ħ ω0 Îz with the z axis aligned with the magnetic field B0, where γ is the gyromagnetic ratio of the nucleus, ω0 is the Larmor frequency of the bare nucleus in radians per second, and ħ is Planck’s constant divided by 2 π radians.

Nb (ω1 >> δ). The behavior is simple as long as ω1 >> δ. For example, if δ = 0, a 90° or π/2 rf pulse has a duration τ90 defined by π/2 = ω1 τ90. , chemical shift) of δ radians s−1. In the next cells, the net magnetization vector Mrot is introduced, the equilibrium net magnetization vector M0 and relaxation matrix R are defined. Then the Bloch equation for the rate of change dMdt is introduced, expanded with the built‐in Expand function, and expressed as a vector using the built‐in MatrixForm function.

### A Primer of NMR Theory with Calculations in Mathematica by Alan J. Benesi

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