By Josquin des Pres

ISBN-10: 0634028561

ISBN-13: 9780634028564

The low, throbbing beat of serious bassists like James Jamerson, Anthony Jackson, Larry Graham, Bootsy Collins, Louis Johnson and Verdine White drove the realm to the dance flooring in the course of the disco period. during this new Bass developers ebook, well known bassist Josquin des Pres offers one zero one actual funk and disco bass styles to assist avid gamers perform getting their groove. comprises regular notation and tab, and a CD with ninety nine full-demo tracks.

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Extra resources for 70s Funk & Disco Bass: 101 Groovin' Bass Patterns

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The position of the carrier frequency has been indicated on the F1 axis. e. similar magnitudes for the rf offset from the carrier frequency. An example of such a case in Figure 90~ T of ~ 2, for the nucleotide 2' deoxycytidine. The pulse scheme -t -SL - acquire(t ) has been employed, with standard phase cycling 1 Y 2 (Table 1) to allow a hypercomplex Fourier transformation (13,16,17) for obtaining an absorption mode 2D spectrum. In this experiment the carrier frequency has been posi tioned in the center of the 3', 4' and 5', 5" region and a 100 ms spin lock pulse with a rf field strength of approximately 6 kHz has been used.

Prolong this The best we have been able to achieve, so far, is a "spin lock" period using a MLEV16 composite pulse decoupling cycle (31), instead of the phase al ter- nated spin lock field (Fig. 3d). A single MLEV-16 cycle consists of a repetitive series of 16 composite pulses, A and B, applied in the order: AABB ABBA BBAA BAAB. y axis. magnetization vectors, 180 Y x , 90 The net effect of A or B • -y -x about the +y (A) or -y (B) axis. Thus, the MLEV 0 0 0 rapidly However, phase alternating spin lock composite pulses A and B rotate initially parallel to the y axis, through space in such a way that effectively one half of the time the magnetization is aligned along the static magnetic xation is determined by T1 , field.

In this expression Hand H denote the effective rf field strengths, experienced by 11 IS spins I and S, and and"S are the respective magnetogyric ratios. "1 Under this condition complete magnetization exchange between two coupled spins occurs in a time I/J IS . This Hartmann-Hahn magnetization transfer mechanism is the basis of heteronuclear cross polarization in solids (12), and has also been applied in ID and 2D heteronuclear NMR experiments in liquids (13,14). (I)); so despite its elegance the method has found little use in liquids.

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70s Funk & Disco Bass: 101 Groovin' Bass Patterns by Josquin des Pres


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