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Alternating magnetic fields

There are two kinds of ultrasonic transducers the magneto-strictive type and the piezoelectric type. The former consists of a metal rod placed in a coil driven by oscillator signals. The alternating magnetic field alternately elongates and compresses the rod. With one end of the rod fixed and the other end connected to a diaphragm, ultrasonic sound waves are produced. [Pg.112]

Due to the orthogonal position of the emission and reception coils, the voltage induced by the alternative magnetic field of emission in the reception coil is zero, so that this will only detect the diffracted magnetic field. [Pg.376]

An alternative way of measuring F(D) is to control forces using magnetic fields instead of controlling... [Pg.1732]

Alternatively, ions of any one selected m/z value can be chosen by holding the magnetic field steady at the correct strength required to pass only the desired ions any other ions are lost to the walls of the instrument. The selected ions pass through the gas cell and are detected in the singlepoint ion collector. If there is a pressure of a neutral gas such as argon or helium in the gas cell, then ion-molecule collisions occur, with decomposition of some of the selected incident ions. This is the MS/MS mode. However, without the orthogonal TOF section, since there is no further separation by m/z value, the new ions produced in the gas cell would not be separated into individual m/z values before they reached the detector. Before the MS/MS mode can be used, the instrument must be operated in its hybrid state, as discussed below. [Pg.159]

Induction furnaces utilize the phenomena of electromagnetic induction to produce an electric current in the load or workpiece. This current is a result of a varying magnetic field created by an alternating current in a cod that typically surrounds the workpiece. Power to heat the load results from the passage of the electric current through the resistance of the load. Physical contact between the electric system and the material to be heated is not essential and is usually avoided. Nonconducting materials cannot be heated directiy by induction fields. [Pg.126]

Inductive interference the production of electrical potentials in conductors due to the induction from alternating magnetic fields arising from short-circuit currents or operational currents in high-voltage power lines. [Pg.505]

Calculation of long-term interference voltages is involved with a multiconductor problem which, in contrast to the short-term interference that derives from a one-pole grounding short circuit, in this case is related to the superposition of alternating magnetic fields of all the conductors of one or several three-phase systems as well as the ground wire. [Pg.519]

Figure 8 Effects of spin diffusion. The NOE between two protons (indicated by the solid line) may be altered by the presence of alternative pathways for the magnetization (dashed lines). The size of the NOE can be calculated for a structure from the experimental mixing time, and the complete relaxation matrix, (Ry), which is a function of all mterproton distances d j and functions describing the motion of the protons, y is the gyromagnetic ratio of the proton, ti is the Planck constant, t is the rotational correlation time, and O) is the Larmor frequency of the proton m the magnetic field. The expression for (Rjj) is an approximation assuming an internally rigid molecule. Figure 8 Effects of spin diffusion. The NOE between two protons (indicated by the solid line) may be altered by the presence of alternative pathways for the magnetization (dashed lines). The size of the NOE can be calculated for a structure from the experimental mixing time, and the complete relaxation matrix, (Ry), which is a function of all mterproton distances d j and functions describing the motion of the protons, y is the gyromagnetic ratio of the proton, ti is the Planck constant, t is the rotational correlation time, and O) is the Larmor frequency of the proton m the magnetic field. The expression for (Rjj) is an approximation assuming an internally rigid molecule.

See other pages where Alternating magnetic fields is mentioned: [Pg.91]    [Pg.19]    [Pg.6]    [Pg.131]    [Pg.111]    [Pg.369]    [Pg.2812]    [Pg.111]    [Pg.294]    [Pg.177]    [Pg.35]    [Pg.323]    [Pg.269]    [Pg.172]    [Pg.780]    [Pg.385]    [Pg.91]    [Pg.19]    [Pg.6]    [Pg.131]    [Pg.111]    [Pg.369]    [Pg.2812]    [Pg.111]    [Pg.294]    [Pg.177]    [Pg.35]    [Pg.323]    [Pg.269]    [Pg.172]    [Pg.780]    [Pg.385]    [Pg.64]    [Pg.342]    [Pg.653]    [Pg.958]    [Pg.1470]    [Pg.1561]    [Pg.435]    [Pg.183]    [Pg.242]    [Pg.322]    [Pg.261]    [Pg.42]    [Pg.190]    [Pg.151]    [Pg.16]    [Pg.11]    [Pg.401]    [Pg.425]    [Pg.212]    [Pg.410]    [Pg.125]    [Pg.131]    [Pg.81]    [Pg.1795]    [Pg.143]    [Pg.288]    [Pg.462]   


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Alternating fields

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