# Magnetics Design Chat: Part 2, Maximum Transfer Power Through Magnetics Components

In the last chat, Magnetics Design Chat: Part 1, Optimal Design of Magnetics Components, our goal was to maximize transfer-power density in a magnetic component so that for a given maximum power, the component is as small as possible. The basic formula for transfer of power through a magnetic core was expressed by the simple relationship:

The two basic limitations on cores are:

This basic conclusion is so important, it bears repeating in another way:

Optimal Turns

The magnetic (core) and electric (winding) designs are connected through the choice of number of turns, N of winding, a central magnetic design parameter. Maximum core transfer-power density, or core utilization , determines turns limits. The turns minimum is NÎ» :

Î”Ď† (p&#772c ) = Î”B(p&#772c )A , where A is the core magnetic path cross-sectional area. Both A and magnetic path length, l , are given in core catalogs along with core magnetic volume, V . The maximum turns is limited by saturation:

The current referred to or â€śseenâ€ť by the core field is Ni&#772 = Nâ‹…i&#772 , where iĚ„ is the average current; Ni&#772 = H&#772â‹…l . It sets the magnetic op-pt and the extent of saturation through ksat .

• Maximum turns that fit winding window, Nw , is another turns limitation â†’ allowable current density

The range of N is bounded by power-loss and saturation limits, and maximum window turns:

With adequate window area for turns, the design range of N is bracketed by core power-loss (NÎ» ) and saturation (Ni ). The core is fully utilized when NÎ» = Ni :

where circuit flux, Î”Î» = Vp â‹…ton , Ip = average (primary) winding on-time current amplitude and Vp = average (primary) winding on-time voltage amplitude. The condition for Nopt is

Solve for the primary-winding on-time power amplitude for the circuit,

where Vp and Ip are the values during on-time, when the primary winding is driven. The on-time power relates to the average primary power, P&#772p , by the duty-ratio, D , the fraction of the switching cycle that is the on-time: ton = Dâ‹…Ts = D /fs and 1/ton = fs /D . Substitute

and core volume,

Then

Then relating to on-time circuit power,

Average power transferred = on-time power, Pp , times the fraction of its duration, D , or

We have maximized P&#772p by equating the turns limits: NÎ» = Ni , where NÎ» is the power-loss minimum N and Ni is the saturation-limited maximum N .

In the next chat, we will look at the circuit-design consequences of these new-found criteria for magnetics design.

## 0 comments on “Magnetics Design Chat: Part 2, Maximum Transfer Power Through Magnetics Components”

This site uses Akismet to reduce spam. Learn how your comment data is processed.