Passive Components Blog
No Result
View All Result
  • Home
  • News
    • All
    • Aerospace & Defence
    • Antenna
    • Applications
    • Automotive
    • Capacitors
    • Circuit Protection Devices
    • electro-mechanical news
    • Filters
    • Fuses
    • Inductors
    • Industrial
    • Integrated Passives
    • inter-connect news
    • Market & Supply Chain
    • Market Insights
    • Medical
    • Modelling and Simulation
    • New Materials & Supply
    • New Technologies
    • Non-linear Passives
    • Oscillators
    • Passive Sensors News
    • Resistors
    • RF & Microwave
    • Telecommunication
    • Weekly Digest

    August 2026 Interconnect, Passives and Electromechanical Components Market Insights

    AEM Introduced High-Power Fuses for Compact Automotive and Industrial Overcurrent Protection

    Knowles Cornell Dubilier 105C Flatpack Aluminum Electrolytic Capacitors Target Low-Profile High-Density Power Designs

    Vishay Thin Film Chip Resistors Combine up to 50 GHz Operation with High Power Density

    Samsung Electro-Mechanics Secures KRW 1.0722 Trillion AI Server MLCC Supply Contract

    KYOCERA AVX Adds 0201 C0G RF MLCCs to KGU Ultra-Low-ESR Capacitor Series

    Vishay Extends High-Current Common-Mode Chokes with 30 A EMI Filtering up to 150 °C

    Bourns Copper-Electrode MOV Series Targets High-Energy Line Surge Protection

    Bourns Expands 12 mm SMD Incremental Encoder with Shaft-Length Options for Compact HMI Controls

    Trending Tags

    • Ripple Current
    • RF
    • Leakage Current
    • Tantalum vs Ceramic
    • Snubber
    • Low ESR
    • Feedthrough
    • Derating
    • Dielectric Constant
    • New Products
    • Market Reports
  • Knowledge Blog
  • Dossiers
    • AI Hardware Dossier
    • Automotive Dossier
    • Industrial Robotics Dossier
    • Power Converter Dossier
    • Capacitor Dossier
    • Resistor Dossier
    • Inductor Dossier
    • Circuit Protection Dossier
  • Suppliers
    • Who is Who
  • PCNS
    • PCNS 2025
    • PCNS 2023
    • PCNS 2021
    • PCNS 2019
    • PCNS 2017
  • Events
  • Home
  • News
    • All
    • Aerospace & Defence
    • Antenna
    • Applications
    • Automotive
    • Capacitors
    • Circuit Protection Devices
    • electro-mechanical news
    • Filters
    • Fuses
    • Inductors
    • Industrial
    • Integrated Passives
    • inter-connect news
    • Market & Supply Chain
    • Market Insights
    • Medical
    • Modelling and Simulation
    • New Materials & Supply
    • New Technologies
    • Non-linear Passives
    • Oscillators
    • Passive Sensors News
    • Resistors
    • RF & Microwave
    • Telecommunication
    • Weekly Digest

    August 2026 Interconnect, Passives and Electromechanical Components Market Insights

    AEM Introduced High-Power Fuses for Compact Automotive and Industrial Overcurrent Protection

    Knowles Cornell Dubilier 105C Flatpack Aluminum Electrolytic Capacitors Target Low-Profile High-Density Power Designs

    Vishay Thin Film Chip Resistors Combine up to 50 GHz Operation with High Power Density

    Samsung Electro-Mechanics Secures KRW 1.0722 Trillion AI Server MLCC Supply Contract

    KYOCERA AVX Adds 0201 C0G RF MLCCs to KGU Ultra-Low-ESR Capacitor Series

    Vishay Extends High-Current Common-Mode Chokes with 30 A EMI Filtering up to 150 °C

    Bourns Copper-Electrode MOV Series Targets High-Energy Line Surge Protection

    Bourns Expands 12 mm SMD Incremental Encoder with Shaft-Length Options for Compact HMI Controls

    Trending Tags

    • Ripple Current
    • RF
    • Leakage Current
    • Tantalum vs Ceramic
    • Snubber
    • Low ESR
    • Feedthrough
    • Derating
    • Dielectric Constant
    • New Products
    • Market Reports
  • Knowledge Blog
  • Dossiers
    • AI Hardware Dossier
    • Automotive Dossier
    • Industrial Robotics Dossier
    • Power Converter Dossier
    • Capacitor Dossier
    • Resistor Dossier
    • Inductor Dossier
    • Circuit Protection Dossier
  • Suppliers
    • Who is Who
  • PCNS
    • PCNS 2025
    • PCNS 2023
    • PCNS 2021
    • PCNS 2019
    • PCNS 2017
  • Events
No Result
View All Result
Passive Components Blog
No Result
View All Result

USB PD 3.0 Flyback Transformer Optimisation

30.1.2023
Reading Time: 8 mins read
A A

In this blog article Sotiris Zorbas, MSc, Frenetic power electronics engineer, suggests USB PD 3.0 compatible flyback transformer optimisation, and how to select the best fit core type using the Core Optimizer™️ tool in Frenetic Magnetics design software.

Let’s consider the drawbacks of flyback transformer designs as in example of Frenetic EQ25 design (Figure 1.):

RelatedPosts

Designing a USB Type‑C Flyback Planar Transformer with Frenetic’s Planar Tool

Designing a Custom Core Transformer for 10 kW LLC Data Center Power Stages

Magnetics Design in High‑Frequency GaN Converters

1. Flying leads at the secondary side

For those of you that haven’t heard of this before, that’s just one design choice when we have a winding ending. There are two options:

  • Terminate the wire to the coil former pin.
  • Leave some cm of extra wire to solder it directly to the PCB. Although this might seem like a simple design choice, the truth is that doing so creates extra manual labour when it comes to the assembly of the PCB board the flyback transformer will be mounted on to. Human intervention is costly!
Figure 1. Frenetic EQ25 USB PD 3.0 Flyback Transformer (conventional “old” design)

Question: Why do we need flying leads in the first place?

Answer: There are a couple of reasons to go for flying leads. In low power transformers/inductors, the reason is high voltages. For a transformer to pass safety standards and be safe to use, many times the distances of the pins between themselves, or with respect to the core, are not enough. For high power applications, the current levels resulting in the use of big wire dimensions create mounting issues. Up to certain wire dimensions things are simple, and the wires can be soldered to the pins. After a point though, that is not an option anymore and flying leads is the decision to go for.

For the flyback design we’re analysing, the problem is high voltages (up to 375VDC in the primary side). Reinforced insulation was selected and, based on IEC61558-1 automotive standard, >6mm of creepage distance is necessary to pass regulation. The EQ25 design shown in Figure 1 can’t pass the standard, if we terminate the secondary winding to the pins, so flying leads are necessary here.

2. Insulating tape for the core (externally)

Just to remind the situation here, the core itself is made of ferrite. We have a primary and a secondary winding. We insulate the primary and/or the secondary to achieve isolation, comply with the standards and pass Hi-pot testing. But the core itself is considered an electrically conductive material, unless coated with insulation, which is not the case with ferrites.

Therefore, we have a conductive material between isolated windings. The transformer will develop some potential if left floating. A solid design choice is to ground the core, either from it clips or by using some copper tape. Conducted EMI is lowered with this design choice.

Question: At which ground should I ground the core?

Answer: We have 2 grounds in USB-PD 3.0 flyback design. The input ground (which is floating – lethal voltages!) and the output ground (safe to touch). Electrically I don’t find a very good reason why grounding the core to one of the grounds is a better option. But I do find that grounding the core at the secondary – safe to touch – ground is a much better option for obvious reasons!

Figure 2. Flyback design – grounds

Without getting into more details, I’ll say that the wire insulation choices at the primary-secondary will either leave the core grounding options open or limit us to a specific choice.

That is the drawback of the EQ25 design. Grounding the core at the secondary side is not allowed, and we are forced to ground the core on the primary side ground. Insulating tape all around the core is needed, being careful to completely cover the ferrite core.

3. Available coil formers.

Unfortunately, the EQ family is not a standard part. EQ cores are planar cores, and that limits the options of coil formers significantly.

Planar cores are called that way because they are designed for planar transformers. That does not exclude them from the classic coil former style approach. The reverse is also applicable. We can design a planar transformer using standard cores. What’s the price of these choices? Availability issues and a limited range of components choices.

The improved design

Assuming the problems of the previous design, I decided to work on a better version, trying to respect most specs of the previous design to be compatible. The design goals of the new transformer are:

  • No flying leads (solve drawback No1)
  • Core can be grounded on the secondary side ground (solve drawback No2)
  • Standard core (solve drawback No3)
  • Maximum power raised at 100W (previous design at 60W)

Let’s focus now on the core selection process. Other aspects of the design will be discussed in the next Newsletters, so stay tuned!

To start the design, I used the Core Optimizer™️ feature of our magnetics design program. This new powerful tool available in Frenetic Online is helping engineers find the appropriate core for a particular application without having to rely on experience and empirical formulas.

Step 1. Decide on the core family/dimensions

As shown in Figure 3, different families of cores were plotted in a volume-primary turns graph. Using height as the deciding factor, I selected the ETD29/16/10 core. To be honest, other similar high options were also available, but they were excluded because of insulation reasons, that have to do with the non-flying lead design choice, made for this design.

Having the ETD29/16/10 core in mind, I moved on to the second graph of the Core Optimizer, that gave me a clear perspective of the core losses under different operating conditions (worst case scenarios).

Figure 3. Core Optimizer™️
Figure 4. Core losses of different materials – same operating conditions

Step 2. Decide on the core loss target

Core loss target set at <0.5W. Three core materials were selected (for ETD29/16/10). Plotting the core losses under the same operating conditions (worst case scenario), we got the following graph shown in Figure 4.

Figure 5. Core losses at different operating conditions

We see a difference of ~0.1W between 50-100 turns for 3C95-3C97. That’s not a lot and both materials could be used. On the other hand, N87 material is not a good option here, having almost x2 power losses. So I picked the 3C97 material.

Step 3. Decide on the number of turns

In Figure 5, having selected 3C97 material, the core losses are shown for different operating conditions. The worst-case scenario, as far as the core losses are concerned, is the combination of 265VAC input voltage and output power at 100W. Selecting 54 turns would be ok for losses <0.5W, but in the end I chose 56 turns to make sure the turns ratio (Np/Ns = 7) would result in an integer number of secondary turns.

The New ETD29 Transformer Design

You can have a look now at the new ETD29 transformer design in Figure 6. and online with details here.

The table 1. shows the specs and differences between the old and new design.

Figure 6. New Frenetic ETD29 USB PD 3.0 Flyback Transformer
Table 1. Frenetic ETD29 (new) vs EQ25 (old) USB PD 3.0 Flyback Transformer Specification comparison

References

[1]  Applications Engineering Department, “Reference Design Report for a 65 W Power Supply Using InnoSwitchTM3-EP PowiGaNTM INN3679C-H606”, Power Integrations 

Related

Source: Frenetic

Recent Posts

August 2026 Interconnect, Passives and Electromechanical Components Market Insights

4.9.2026
4

Vishay Extends High-Current Common-Mode Chokes with 30 A EMI Filtering up to 150 °C

3.9.2026
14

B–H Curve-Based Inductor Modelling in LTspice: A Current-Dependent Magnetic Model

31.8.2026
34

Vishay IFBT SMT Flyback Transformers Target PoE and Isolated DC/DC Designs up to 30 W

28.8.2026
20

Bourns Automotive BMS Signal Transformer Combines Reinforced Isolation and Common-Mode Noise Rejection

27.8.2026
27

Vishay Introduces Automotive Low Loss SMD Common-Mode Chokes

26.8.2026
33

Current-Dependent Inductors: Using Non-Linear Inductance in Buck Converters and PFC Stages

24.8.2026
43

Passive Components for Industrial Automation and Robotics (Dossier Report 08/26)

20.8.2026
125

Single Pair Ethernet for Humanoid Robot In-Robot Networks

17.8.2026
179

Upcoming Events

Sep 10
11:00 - 12:00 CEST

Equipment models and model strategies for Space Missions

Sep 16
17:00 - 18:00 CEST

Designing a 5 kW, 800 V-to-50 V PSFB Converter for Next-Generation Data Centers

Sep 29
16:00 - 17:00 CEST

Cybersecurity 2026

View Calendar

Popular Posts

  • Buck Converter Design and Calculation

    0 shares
    Share 0 Tweet 0
  • LLC Resonant Converter Design and Calculation

    0 shares
    Share 0 Tweet 0
  • Boost Converter Design and Calculation

    0 shares
    Share 0 Tweet 0
  • Earthing Systems and IEC Classification Explained

    0 shares
    Share 0 Tweet 0
  • MLCC and Ceramic Capacitors

    0 shares
    Share 0 Tweet 0
  • Flyback Converter Design and Calculation

    0 shares
    Share 0 Tweet 0
  • Capacitor Charging and Discharging

    0 shares
    Share 0 Tweet 0
  • Audio Capacitors: Choosing Capacitors for Crossover Circuits

    0 shares
    Share 0 Tweet 0
  • Resistor Symbols

    0 shares
    Share 0 Tweet 0
  • Thermistors Basics, NTC and PTC Thermistors

    0 shares
    Share 0 Tweet 0

Newsletter Subscription

 

Passive Components Blog

© 2015–2026
All rights reserved

  • Home
  • Privacy Policy
  • EPCI Membership & Advertisement
  • About

No Result
View All Result
  • Home
  • Knowledge Blog
  • Dossiers
  • PCNS

© 2015–2026
All rights reserved