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  2. Ch 6-9 probs /2

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_6_9_probs.pdf
    24 Feb 2004: b 30 and 60 transferred to 30. c 60 transferred to 30 and 60. ... You will need theidentity cos sin sin sinA B B A B A= ( ) ( )[ ]12 ]. E7-6. Consider the COSY spectrum for a three-spin system. Start withmagnetization just on spin 1.
  3. C:/Documents and Settings/jhk10/My Documents/NMR Course 2004/../NMR…

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_3.pdf
    24 Feb 2004: Under these circumstances the offset, , is zero and so the reducedfield, B, is also zero. ... 3.10 Relaxation 3–15. xy y. z. B1. x. z. B1. (a) (b).
  4. Chapter 7/3(A4)

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_7.pdf
    24 Feb 2004: modulation in t1 can be expanded, using the formula,cos sin sin sinA B B A B A= ( ) ( ){ }12 to give. ... If two two-dimensional multipletsappear at (F1, F2) = (A B, A) and (A B, B) the implication is thatthe two spins A and B are coupled, as it is only
  5. Chapter 9 a4 /2

    https://www-keeler.ch.cam.ac.uk/lectures/understanding/chapter_9.pdf
    24 Feb 2004: Fouriertransformation of S(t) gives the spectrum S(ω):. S B A Dω ω ω( ) = ( ) ( )[ ] ( )i iexp Φ [1]. ... Re cos sinS B A Dω ω ω( )[ ] = ( ) ( )[ ]Φ ΦIn general this is a mixture of the absorption and dispersion lineshape.

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