Previous Page  18 / 84 Next Page
Information
Show Menu
Previous Page 18 / 84 Next Page
Page Background

Figure 1: Outer package and core structure: core material losses

are reduced with the WE-MAPI coil

Figure 2: REDEXPERT User-Interface: the online tool calculates

ideal power inductance and estimates temperature

the core and soldered or welded to

the terminal with a clip. The outer

shielding ring is then mounted and

bonded with the inner core and the

winding. WE-MAPI is different: the

winding is contacted directly with

the component's connection pad

without soldering and welding. By no

longer requiring the clip, the effective

diameter was increased, thus

requiring fewer windings for the same

inductance values. This is directly

expressed in a considerably reduced

DC resistance (RDC) of the winding.

The core of WE-MAPI consists of an

innovative metal alloy pressed around

the winding. This gives the coil high

inductance values with a small package

size. At the same time, a self-shielding

effect is achieved by the special

construction of the core. The core

material itself is temperature stable

with little drift and soft saturation

behavior. A protective layer is also

applied around the core protecting

the surface against environmental

influences.

Losses in power inductors

The losses of power inductors are

driven by a combination of core

material losses and winding losses.

The latter can be divided into DC

current losses, principally influenced

by the DC resistance of the winding

(P=I2* RDC) and the AC losses (RAC)

of the winding that result from skin

and proximity effects.

In switching controllers, the coil is one

of the most important components

and therefore, accurate determination

of losses and heating is a key step in

the selection of the right component.

To predict heating, the AC losses must

be accurately determined first. Here,

the Dowell-, Ferreira- or Nan/Sullivan

methods are just some of the methods

used today.

Historically, core losses were

determined using the Steinmetz

model, and later with a modified or

generalizedSteinmetzmodel. Themain

drawback of the Steinmetz equation

is that it mainly applies for sinusoidal

excitations and determination of the

coefficients is usually only measured

with small signals. However, for most

applications in power electronics, the

coil current is not sinusoidal. And the

currents are large signals of several

milliamps (mA) up to several hundred

18 l New-Tech Magazine Europe