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Magnetic force measurement

Typical correlation between the magnetic characteristic and the body force measured on the head of 85 mm long M24 Friedberg 10.9 bolts where the thickness off the plates screwed together is more than 40mm. [Pg.6]

A wide variety of measurements can now be made on single molecules, including electrical (e.g. scanning tunnelling microscopy), magnetic (e.g. spin resonance), force (e.g. atomic force microscopy), optical (e.g. near-field and far-field fluorescence microscopies) and hybrid teclmiques. This contribution addresses only Arose teclmiques tliat are at least partially optical. Single-particle electrical and force measurements are discussed in tire sections on scanning probe microscopies (B1.19) and surface forces apparatus (B1.20). [Pg.2483]

An additional, independent estimate of the concentration of paramagnetic superoxo and diamagnetic hydroperoxo-/peroxo-titanium species was made from magnetic susceptibility measurements using a Lewis coil force magnetometer (52). The gram-susceptibility of Ti in TS-1 + H2C>2 was estimated to be 5.5 X 10-6 emu/g, which corresponds to an effective magnetic moment of... [Pg.69]

At resonance, the magnetization vector M precesses about the vector B, i of the alternating field according to eq. (1.34). As a result, a component of transverse magnetization My.j rotates in the x y plane at the Larmor frequency v0. If a receiver coil is placed in the x y plane, the rotating magnetic vector Myj induces an electromotive force measurable as an inductance current. This process is called nuclear induction [5, 8]. The orientation of the coil axis will affect the phase relative to B1 i but not the magnitude of the induction current. [Pg.13]

Let us turn now to the other conclusions which can be based on free electron theory. The Hall effect measurements of Kyser and Thompson permitted the computation of the free electron concentration. The Hall effect is produced by a balance between the magnetic force (Lorentz force) on a current carrier and the electric force produced by a displaced charge density within a conductor. For a charge, q, moving... [Pg.108]


See other pages where Magnetic force measurement is mentioned: [Pg.214]    [Pg.214]    [Pg.49]    [Pg.214]    [Pg.214]    [Pg.49]    [Pg.1733]    [Pg.177]    [Pg.182]    [Pg.401]    [Pg.284]    [Pg.201]    [Pg.782]    [Pg.1029]    [Pg.670]    [Pg.82]    [Pg.18]    [Pg.27]    [Pg.78]    [Pg.352]    [Pg.146]    [Pg.360]    [Pg.72]    [Pg.87]    [Pg.40]    [Pg.53]    [Pg.207]    [Pg.19]    [Pg.433]    [Pg.247]    [Pg.419]    [Pg.78]    [Pg.553]    [Pg.959]    [Pg.960]    [Pg.177]    [Pg.182]    [Pg.423]    [Pg.294]    [Pg.91]    [Pg.190]    [Pg.16]    [Pg.566]    [Pg.200]    [Pg.53]    [Pg.282]    [Pg.365]   
See also in sourсe #XX -- [ Pg.85 ]

See also in sourсe #XX -- [ Pg.85 ]




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