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Toroidal inductors and transformers are inductors and transformers which use magnetic cores with a toroidal (ring or donut) shape. They are passive electronic components , consisting of a circular ring or donut shaped magnetic core of ferromagnetic material such as laminated iron , iron powder, or ferrite , around which wire is wound.
The ferrite cores used for power transformers work in the low-frequency range (1 to 200 kHz usually [2]) and are relatively large in size, can be toroidal, shell, or shaped like the letters 'C', 'D', or 'E'.
Thus, when using frequencies higher than 500 kHz MPP cores are often replaced by ferrite cores. [4] Disadvantages of MPP cores: Due to the complex nature of its manufacturability and tooling feasibility, shapes are limited to a toroidal configuration and these types of cores generally have maximum operating frequency of around 1 MHz.
A choke is an inductor designed specifically for blocking high-frequency alternating current (AC) in an electrical circuit, while allowing DC or low-frequency signals to pass. Because the inductor restricts or "chokes" the changes in current, this type of inductor is called a choke.
A variable-frequency transformer is a specialized three-phase power transformer which allows the phase relationship between the input and output windings to be continuously adjusted by rotating one half. They are used to interconnect electrical grids with the same nominal frequency but without synchronous phase coordination.
Toroidal transformer - the core is in the shape of a toroid. This is a commonly used shape as it decreases the leakage flux, resulting in less electromagnetic interference. Induction coil or trembler coil - an early transformer which uses a vibrating interrupter mechanism to break the primary current so it can operate off of DC current.
In electromagnetism, a toroidal moment is an independent term in the multipole expansion of electromagnetic fields besides magnetic and electric multipoles. In the electrostatic multipole expansion, all charge and current distributions can be expanded into a complete set of electric and magnetic multipole coefficients.
In practice, an instrument will use a lossy integrator with a time constant much less than the lowest frequency of interest. The lossy integrator will reduce the effects of offset voltages and set the constant of integration to zero. At high frequencies, the Rogowski coil's inductance will decrease its output. The inductance of a toroid is [8]
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