Current Sense Transformer Calculation and Application

This paper provides a comprehensive overview of current sense transformer (CST) technology, from operating principles and calculation methods to practical implementation in switched‑mode power supplies (SMPS) and automotive systems.

It begins with the fundamentals of CST operation, compares current sensing technologies across the frequency spectrum, and then develops a step‑by‑step design and calculation methodology based on YAGEO Group technical data. An integrated application section uses Coilcraft SMPS design material to illustrate CST behavior, core reset, and design trade‑offs in real controllers and reference designs.

Key Takeaways

  • CSTs provide high‑accuracy, galvanically isolated, low‑loss current measurement, especially suited for high‑frequency AC and SMPS applications.
  • Compared with shunt resistors, Hall‑effect sensors, and Rogowski coils, CSTs offer an excellent balance of isolation, efficiency, and EMI robustness in the high‑frequency domain, but they cannot sense DC.
  • Correct CST selection is driven by RMS current rating, volt‑second product/flux density, turns ratio, terminating resistor, isolation rating, and mechanical constraints.
  • A 3‑step selection flow (series choice, part number choice, error and delay analysis) enables fast and robust CST design.
  • Case studies from automotive BMS and SMPS controllers demonstrate that well‑designed CSTs can achieve sub‑percent amplitude and phase errors over the intended frequency range.

Introduction

As energy efficiency becomes a defining requirement for modern electronic systems, the ability to measure current with high precision has never been more critical. Accurate current monitoring enables engineers to optimize power conversion, detect faults, and guarantee compliance with stringent safety standards.

Different application domains call for different sensing strategies. Broadly, current sensing can be divided into three categories:

Current-frequency domain

Fig. 1) Usage of Current Sense Transformers in Current-Frequency Domain

While several sensing technologies are available—including shunt resistors, Rogowski coils, and current sense transformers (CSTs)—the CST stands out when accuracy, galvanic isolation, and efficiency at high frequencies are essential.

Technology landscape: Comparing sensing methods

Selecting the right current sensing technology requires balancing trade-offs in accuracy, cost, power dissipation, isolation, and frequency response.

TechnologyAdvantagesLimitationsTypical applications
Shunt resistorLow cost, simple, no phase errorHigh loss, no isolationLow-power DC/DC, battery monitoring
Hall-effect sensorHigh accuracy, galvanic isolation, DC & AC sensingExpensive, requires power, temperature sensitiveIndustrial drives, medical, precision systems
Current sense transformer (CST)Accurate, low-loss, isolated, good EMI immunityNo DC response, core saturation at very low frequencySMPS, AC line monitoring, solar/UPS
Rogowski coilWide bandwidth, no core saturation, high currentNeeds integrator, poor low-frequency responseTransient analysis, arc fault detection, power quality

Every CST has a minimum usable frequency below which phase shift and amplitude error become unacceptable for control purposes. As frequency decreases, the induced secondary voltage becomes small relative to magnetizing current and burden resistor effects, which leads to increasing phase lag and distortion; true DC components are not transferred but still bias the core flux and can cause flux walking toward saturation if not reset.

The decision often comes down to whether the application requires high efficiency and strong isolation at high frequency—an area where CSTs consistently outperform alternatives.

Application domains

CSTs are widely adopted wherever high‑frequency AC current must be monitored efficiently and safely.

Figure 2. Typical current sense transformer application schematic Source: Coilcraft Doc1288 Current Sensor Selection

Typical domains include:

Operating Principles of Current Sense Transformers

The operation of a current sense transformer is grounded in the fundamentals of electromagnetic induction. When an AC current flows through the primary winding, it induces a proportional current in the secondary. This secondary current, when passed through a terminating resistor, produces a measurable voltage directly proportional to the original current.

Ideal relationships

(1) Sense current vs. primary current (ideal CST)

IPrim=N⋅IsenseI_{\text{Prim}} = N \cdot{I_{\text{sense}} }

Where N means a turn-ratio. Voltage sense is a direct measurement of a primary current Iprim

(2) Sense voltage across terminating resistor

Vsense=RT⋅IprimNV_{\text{sense}} = R_T \cdot \frac{I_{\text{prim}}}{N}

Non-ideal behavior and losses

Flowing primary current slightly differs from measured current value, as the core of current sense transformers needs to be magnetized by magnetizing current. Hysteresis losses (IFe) are typically negligible for CSTs. The magnetizing current can be identified from basic parameters as a source of amplitude error.

(3) Primary current composition

Iprim=Imeas−ImagI_{\text{prim}} = I_{\text{meas}} – I_{\text{mag}}
Fig. 3a) Simplified Operating Principle of CST; Fig 3b) right: Example photographs of CST products

Magnetic modeling and optimization

Imag=(VSenseN)⋅dutycycleLm[mH]⋅Freq[kHz]I_{\text{mag}} = \frac{\left( \frac{V_{\text{Sense}}}{N} \right) \cdot \text{duty}_{\text{cycle}}}{L_m\,[\text{mH}] \cdot \text{Freq}\,[\text{kHz}]}

To optimize CST parameters, magnetic Finite Element Method (FEM) analysis is used. Magnetic field distribution analysis helps determine magnetic losses and phenomena related to phase shift between measured and sensed current values.

VSense=RT⋅IPrimN=RT⋅Imeasured−ImagNV_{\text{Sense}} = R_T \cdot \frac{I_{\text{Prim}}}{N} = R_T \cdot \frac{I_{\text{measured}} – I_{\text{mag}}}{N}
Fig. 4) Example magnetic field distribution within CST (shape core version), B [Gauss]

Comparator-based measurement

A CST integrates easily into analog or digital measurement systems. The sense voltage—i.e., the voltage drop across the external terminating resistor RT – is commonly used as the comparator input voltage.

(4) Comparator input and output behavior

Comparator’s tasks is to compare measured Vsense value to assigned reference voltage Vref, where Vref value typically defines maximum voltage drop we can measure on RT – under Isense is flowing:

Vref=max⁡(Vsense)=RT⋅IsenseV_{\text{ref}} = \max(V_{\text{sense}}) = R_T \cdot I_{\text{sense}}

As result – we get final referenced output voltage Vout, which can be directly used for discrete or analog regulation systems or for monitoring purpose.

Fig. 5) Functional electric schematic of CST in measurement circuit with burden resistor RT

Current sense transformer selection guidelines

Accurate and reliable CST implementation depends on proper selection of both the magnetic component and the measurement network.

Key design parameters include:

A practical design flow can be split into three main steps.

Step 1. Product series choice based on safety

The first step is to define application constraints: maximum current, insulation level, operating voltage, and form‑factor limits.

YAGEO catalog CSTs, for example, offer solutions up to about 1.5 kV with appropriate creepage and clearance for reinforced insulation, and package families optimized for continuous currents up to tens of amperes and switching frequencies into the low‑MHz range. Full‑custom CSTs are often used when current exceeds catalog ranges or when non‑standard busbar or PCB geometries are required.

Fig. 6) YAGEO Catalog Product Portfolio range of CST

The catalog portfolio covers mechanically optimized constructions for applications up to 50 A with a wide range of turns ratios. Some products support measurement frequencies up to 2 MHz. Full custom designs are available for wider current ranges.

Step 2 – Part Number Choice, Working Point, and Terminating Resistor

With a suitable series identified, the next step is to select the turns ratio and calculate the operating flux density and burden resistor.

Input Parameters. Typical inputs are:

Working point and flux density

Selection starts with CST turns ratio based on working point (flux density B) under given conditions: frequency (f), duty cycle (D), and Vref. Datasheets specify the effective core area Ae used in flux estimations.

(5) Flux density working point (conceptual)

B[Gauss]=1Ae⋅Vref⋅DutycycleN⋅FreqkHzB\, [\text{Gauss}] = \frac{1}{A_e} \cdot \frac{V_{\text{ref}} \cdot \text{Duty}_{\text{cycle}}}{N \cdot \text{Freq}_{\text{kHz}}}

To stay in the linear part of the core B/H characteristic, the working point B should typically be within 250–2200 Gauss, with the absolute maximum specified in the datasheet. This region determines a feasible solution domain for part selection.

Fig. 7. Example of Flux Density vs. Frequency characteristics for CST calculated for constant Vref condition

Higher frequencies generally require lower turns counts and higher Vref, while lower frequencies require higher turns ratios and may use lower Vref. The turns ratio N impacts sensitivity: higher N lowers the working point and Vsense, reducing sensitivity.

Terminating resistor calculation

Once a part number is selected, determine the terminating resistor value.

(6) Terminating resistor from peak conditions

RT=VSense⋅NIprimR_T = \frac{V_{\text{Sense}} \cdot N}{I_{\text{prim}}}

Step 3. Measurement error, signal delay & sensitivity

Analyze amplitude and phase shift error. Amplitude error is mostly caused by CST losses, where magnetizing current plays a significant role and is typically small and linear (often < 2%). Phase error depends on burden and parasitics and should be minimized during design.

(7) Amplitude error due to magnetizing current

IError[%]=(1−|Imeasured−ImagImeasured|)⋅100%I_{\text{Error}}[\%] = \left(1 – \left| \frac{I_{\text{measured}} – I_{\text{mag}}}{I_{\text{measured}}} \right| \right) \cdot 100\%

(8a) Phase shift (general)

a[Deg]=atan⁡(RT+RDCsec2⋅π⋅FreqkHz⋅L[mH])a[\text{Deg}] = \operatorname{atan} \left( \frac{R_T + R_{\text{DCsec}}}{2 \cdot \pi \cdot \text{Freq}_{\text{kHz}} \cdot L[\text{mH}]} \right)

(8b) Phase shift (simplified when RT ≫ RDC,sec)

a[Deg]=atan⁡(RT2⋅π⋅FreqkHz⋅L[mH])a[\text{Deg}] = \operatorname{atan} \left( \frac{R_T}{2 \cdot \pi \cdot \text{Freq}_{\text{kHz}} \cdot L[\text{mH}]} \right)

(8c) Maximum phase error estimate

Errora[%]=(1−cos⁡a)⋅100%(8c)\text{Error}_a[\%] = (1 – \cos a) \cdot 100\% \tag{8c}

Sensitivity

(9a) Sensitivity (V/A)

sensitivity[V/A]=(Vsense[V]Imeasured[A])\text{sensitivity}\,[\text{V/A}] = \left( \frac{V_{\text{sense}}\,[\text{V}]}{I_{\text{measured}}\,[\text{A}]} \right)

(9b) Sensitivity error

IError[%]=(1−|Imeasured−IimagImeasured|)⋅100%I_{\text{Error}}\,[\%] = \left(1 – \left| \frac{I_{\text{measured}} – I_{\text{imag}}}{I_{\text{measured}}} \right| \right) \cdot 100\%

Case study: High-accuracy CST performance

Consider an automotive current sensing application such as battery management or DC‑DC converter current monitoring, with the following conditions:

A catalog series (for example, YAGEO CSFA family) is selected that meets insulation and size constraints. Within the PMS9494 range, turns ratios of 1:50, 1:100, 1:150, and 1:200 are available; flux‑density calculations show that 1:50 slightly exceeds the recommended 2200 Gauss limit, while 1:100 falls nicely in the mid‑range, leaving margin for variations in frequency, current, and duty cycle.

Using N=100, the burden resistor required at 29 A peak and 15 V reference is approximately:

RT=15⋅10029≈52 Ω

A standard 50 Ω value is a convenient practical choice and keeps the secondary DCR contribution negligible.

Magnetizing current under these conditions is on the order of a fraction of a milliampere, resulting in amplitude error well below 0.01%. Simplified phase‑shift calculations yield roughly 1 degree of phase angle at 200 kHz, corresponding to a phase‑related amplitude error of about 0.0164%, demonstrating the extremely high accuracy achievable with a correctly selected CST.

The resulting sensitivity is:

sensitivity≈14.5 V29 A≈0.5 V/A

showing how burden choice directly sets volts‑per‑ampere gain and influences effective dynamic range at the comparator or ADC input.

Fig. 8) Case study schematics

Designing a Custom Current Sense Transformer

When catalog parts cannot meet the mechanical or current requirements, custom CSTs can be designed around the same principles.

Core Choice – Key considerations include:

Window Utilization – The physical window must accommodate the chosen primary conductor style, secondary winding, insulation layers, and creepage/clearance:

Loss and Temperature – A quick loss and temperature‑rise estimation combines:

These calculations define whether the selected core and winding scheme meet thermal limits across the intended ambient range.

Step 1: Series choice

Automotive applications require functional insulation. With the noted mechanical constraints, select CSFA series and use the YAGEO Group product selector to locate a suitable range.

Fig. 9) Screenshot of YAGEO Group Product Selection Tool

Step 2: Part selection and working point

Open the datasheet to review parameters. In this case, four turns ratios are available for the PMS9494 product range.

Fig. 10) Example of datasheet (Series CSFA – product range PMS9494)

To better understand, we calculate working point based (flux density B) according to Eq.5 based on our automotive application conditions: Freq. = 200kHz, Vref=15V, DutyCycle=0.8. This equation is also specified in datasheet (Fig. 10, Notes, Pkt 4). Calculations can be systemized as in Table 2:

NDutyCycleVref [V]Freq [kHz]Ipk [A]B [Gauss]Rsense [Ω]
500.81520029225625.86207
1000.81520029112857.72414
1500.8152002975277.58621
2000.81520029564103.483

The N=50 option exceeds the suggested limit of B = 2200 Gauss and is excluded. The 1:100 option (PMS9494.100NLT) places B mid-range within the recommended window, providing flexibility for wider switching frequency or overcurrent.

RT=Vref⋅NIpkR_T = \frac{V_{\text{ref}} \cdot N}{I_{\text{pk}}}
RT=(15V⋅100)29A=51,72[Ω] R_T = \frac{(15\,\text{V} \cdot 100)}{29\,\text{A}} = 51{,}72\, [\Omega]

From Eq. (6), the terminating resistor for the selected part is approximately RT ≈ 50 Ω. The secondary winding DCR is < 10% of RT and has negligible influence on phase shift under these conditions.

Error and sensitivity estimates

Previous calculated values of B and RT allows us to calculate the amplitude error of the magnetizing current:

Imag=(VsenseN⋅dutycycle)Lm[mH]⋅FreqkHz I_{\text{mag}} = \frac{\left( \frac{V_{\text{sense}}}{N} \cdot \text{duty}_{\text{cycle}} \right)}{L_m\,[\text{mH}] \cdot \text{Freq}_{\text{kHz}}}
Imag=((14.5100)⋅0.8)÷(2.2⋅200)=0.28mAI_{\text{mag}} = \left( \left( \frac{14.5}{100} \right) \cdot 0.8 \right) \div (2.2 \cdot 200) = 0.28\,\text{mA}

Amplitude error due to magnetizing current is very small. Example calculation yields approximately 0.00154%, indicating the magnetizing current component is not measured.

IError[%]=(1−|Imeasured−ImagImeasured|)⋅100%I_{\text{Error}}[\%] = \left(1 – \left| \frac{I_{\text{measured}} – I_{\text{mag}}}{I_{\text{measured}}} \right| \right) \cdot 100\%
IError[%]=(1−|29−0.002829|)I_{\text{Error}}[\%] = \left(1 – \left| \frac{29 – 0.0028}{29} \right| \right)
100%=0,00154%100\% = 0{,}00154\%

Simplified phase shift calculation indicates a very low signal shift

a[Deg]=tan−1⁡(RT2⋅π⋅FreqkHz⋅L[mH])a\,[\text{Deg}] = \tan^{-1}\left( \frac{R_T}{2 \cdot \pi \cdot \text{Freq}_{\text{kHz}} \cdot L\,[\text{mH}]} \right)
a[Deg]=tan−1⁡(50[Ω]2⋅π⋅200[kHz]⋅2.2[mH])=tan−1⁡(502763)=tan−1⁡(0.018)=1.037∘a\,[\text{Deg}] = \tan^{-1}\left( \frac{50\,[\Omega]}{2 \cdot \pi \cdot 200\,[\text{kHz}] \cdot 2.2\,[\text{mH}]} \right) = \tan^{-1}\left( \frac{50}{2763} \right) = \tan^{-1}(0.018) = 1.037^\circ
Errorα[%]=(1−cos⁡α)⋅100%=(1−0.99984)⋅100%=0.0164% \text{Error}_{\alpha}\,[\%] = (1 – \cos{\alpha}) \cdot 100\% = (1 – 0.99984) \cdot 100\% = 0.0164\%

In this configuration, the measurement error is only 0.0164% and demonstrates exceptional accuracy achievable with well-designed CSTs.

Sensitivity of selected part number under application requirements will be:

sensitivity[V/A]=Vsens[V]Iprim[A]=Isens[A]⋅Rf[Ω]Iprim[A]=14.5[V]29[A]=0.5[V/A]\text{sensitivity}\,[\text{V/A}] = \frac{V_{\text{sens}}\,[\text{V}]}{I_{\text{prim}}\,[\text{A}]} = \frac{I_{\text{sens}}\,[\text{A}] \cdot R_f\,[\Omega]}{I_{\text{prim}}\,[\text{A}]} = \frac{14.5\,[\text{V}]}{29\,[\text{A}]} = 0.5\,[\text{V/A}]
Errorsensitivity[%]=Vsens−VrefVref⋅100%=(14.5−15)15⋅100%=0.033⋅100%=3.3%\text{Error}_{\text{sensitivity}}\,[\%] = \frac{V_{\text{sens}} – V_{\text{ref}}}{V_{\text{ref}}} \cdot 100\% = \frac{(14.5 – 15)}{15} \cdot 100\% = 0.033 \cdot 100\% = 3.3\%

Choice of terminating resistance influence sensitivity and sensitivity error.

Behavior Under Fault and Overload Conditions

Under overload or short‑circuit conditions, both peak flux density in the core and power dissipation in the burden resistor increase significantly.

Important checks include:

Protection schemes often add diodes and clamps to manage reset and overvoltage, as discussed in the SMPS application section below.

PCB Layout and EMC Considerations

Good PCB practice is crucial to preserve CST accuracy and minimize EMI issues.

Key layout rules:

These layout practices are particularly important in SMPS designs, where CST signals interface directly with high‑speed current‑mode controllers.

Application in Switched‑Mode Power Supplies

Current sense transformers are widely used in SMPS controllers to monitor peak or average inductor current with high efficiency and isolation. Here is a practical framework example for deploying CSTs in this role.

Basic SMPS Use Case

In a typical implementation, a 1‑turn primary is formed by the power trace or lead that carries the converter’s inductor or switch current. The CST secondary, with many turns, drives a burden resistor that develops a low‑voltage signal proportional to primary current, which is then fed into a controller’s current sense input.

The basic relationship:

Vout=Ipri⋅RTNsecV_{\text{out}} = \dfrac{I_{\text{pri}} \cdot R_T}{N_{\text{sec}}}

shows that, for a given primary current, the designer chooses RTR_T and NsecN_{\text{sec}} to achieve the desired maximum sense voltage (for example, 1 V/A scaling).

Core Reset and Diode Usage

For high duty‑cycle operation, a key design requirement is ensuring that the CST core is reset each switching period to prevent flux walk and saturation.

A common practice is to place a diode in series with the secondary, across the burden network, so that during the off‑time the core sees a reverse voltage and returns to zero flux, while the reset voltage is isolated from the controller input. A Zener diode may also be added to clamp the secondary voltage during fault conditions and protect both the CST and downstream circuitry.

Without proper reset, residual flux accumulates each cycle, causing the sensed current to appear lower than the true primary current and potentially driving the controller into destructive over‑current conditions.

Turns Ratio Trade‑Offs

Off‑the‑shelf CST families often offer multiple turns ratios in the same package size. Design trade‑offs when choosing a higher versus lower turns ratio include:

Analysis shows that, for a given package, different turns ratios can be optimized to balance efficiency, accuracy, and bandwidth, and that online selection tools can automate flux‑density checking to avoid saturation.

Table 3. Current Transformer Turns Ratio Effects*; source: Coilcraft

SMPS Application Examples

Example 1 – LTC3706 Secondary‑Side Synchronous Forward Controller

Analog Devices’ LTC3706 controller documentation compares CST‑based sensing with resistive methods for high‑efficiency, high‑output‑voltage converters.

Figure 11. Current Transformer: Highest Efficiency, High Vout Capable; Source: Analog Devices, Figure 3D, page 16

In one example, a current sense transformer on the secondary side monitors inductor current in a synchronous forward topology. The CST provides:

The CST sense voltage is fed into the controller’s current sense pin, and the turns ratio plus burden are chosen so that the maximum expected current corresponds to the controller’s internal sensing threshold.

Example 2 – TI TIDM‑02009 EV Traction DC‑DC Converter

Texas Instruments’ TIDM‑02009 ASIL‑D‑assessed traction DC‑DC converter reference design uses two Coilcraft CST2010‑100L 1:100 CSTs to sense primary inductance current in a bidirectional converter linking a 400/600 V bus to a 12 V battery.

The converter employs peak current‑mode control, with the CSTs providing isolated feedback of high‑speed current waveforms. The CSTs are selected to:

This example illustrates how catalog CSTs can be integrated into safety‑critical EV systems using standard design flows and online selection tools.

Integrated Design Considerations

Bringing together the calculation and application perspectives, a practical CST design and selection process for SMPS and automotive systems involves:

  1. Defining electrical, safety, and mechanical requirements (current range, bus voltage, insulation class, ambient and size).
  2. Choosing a CST series and tentative turns ratio that satisfy insulation and size constraints while keeping flux density within the recommended window.
  3. Calculating the burden resistor to map peak current to the desired sense voltage, checking resistor power and controller input limits.
  4. Estimating amplitude and phase errors from magnetizing current and parasitic elements, verifying that they are acceptable over the entire operating frequency range.
  5. Implementing appropriate core reset and secondary protection (diodes, clamps) to prevent flux walk and overvoltage during faults.
  6. Validating performance in circuit through measurements or simulation, and iterating turns ratio or burden value if necessary.

By following this structured flow, designers can confidently exploit the advantages of current sense transformers in high‑performance power converters while avoiding common pitfalls related to saturation, bandwidth, and noise.

Conclusion

Current sense transformers combine high accuracy, galvanic isolation, and low loss, making them a technology of choice for high‑frequency AC current measurement in SMPS, solar inverters, UPS, industrial automation, and automotive systems. With a disciplined selection and calculation process, errors well below 1% in both amplitude and phase are achievable, even in compact, high‑current applications.

As energy efficiency accelerates, CSTs will continue enabling next-generation power systems. CSTs exhibit low measurement error compared to shunts and Rogowski coils due to minimal temperature rise, shielding against external EM fields, and lower energy dissipation than shunts.

FAQ about Current Sense Transformers

What is a Current Sense Transformer (CST)?

A Current Sense Transformer is a transformer optimized for current measurement rather than power transfer, providing galvanic isolation and a low‑loss voltage signal proportional to AC or high‑frequency current. It is widely used in switch‑mode power supplies, solar inverters, industrial drives, and automotive power electronics where efficiency and isolation are critical.

How does a CST compare to other sensing methods?

Compared with shunt resistors, Hall‑effect sensors, and Rogowski coils, CSTs offer very low power dissipation and strong isolation in the high‑frequency domain. They cannot sense DC, but for AC and high‑frequency currents they often provide better efficiency, EMI robustness, and phase accuracy than resistive or Hall‑based solutions.

What are the main application domains of CSTs?

CSTs are mainly used in SMPS and DC‑DC converters for peak or average current‑mode control, in high‑voltage converters for isolated current feedback, and in solar, UPS, industrial automation, and EV powertrains where fast, isolated current measurement is required.

What factors influence CST accuracy?

Accuracy is primarily affected by magnetizing current, core material and flux density, burden resistor value, and parasitic inductances and capacitances, which together determine amplitude and phase error. Careful selection of turns ratio and burden, flux‑density checking, and, where needed, FEM magnetic analysis keep total error typically well below 1% over the intended frequency range.

How do engineers select the right CST?

Designers start from electrical, safety, and mechanical requirements, then choose a product series and turns ratio that satisfy insulation and flux‑density limits. They calculate the terminating resistor from peak current and desired sense voltage, check error and phase shift against the operating frequency range, and finally validate performance in the real SMPS or automotive application.

Can a current sense transformer measure DC?

No, a current sense transformer cannot measure true DC current because it operates on the principle of changing magnetic flux and therefore only responds to AC or high‑frequency components. Any DC component in the primary current does not appear in the secondary signal but still biases the core and can lead to flux walking and eventual saturation if the core is not properly reset each switching cycle.

How to Select a Current Sense Transformer

  1. Step 1: Define application requirements

    Identify current type and range (peak and RMS), switching frequency, and insulation class, together with mechanical limits such as footprint, height, and primary conductor style (PCB trace, wire, or busbar). Confirm any safety requirements for creepage, clearance, and reinforced or functional insulation.

  2. Step 2: Choose product series and part number

    Use the manufacturer’s product selector to pick a CST series that meets isolation and size constraints, then select a tentative turns ratio that keeps core flux density within the recommended window over your duty cycle and switching frequency. This corresponds to Step 1 and Step 2 of the 3‑step selection method described in this article.

  3. Step 3: Calculate terminating resistor

    rom peak primary current and the controller’s maximum sense or comparator reference voltage, calculate the burden resistor so that the highest expected current produces the target sense voltage. Verify that the resistor’s power rating and tolerance are adequate for normal operation and fault conditions.

  4. Step 4: Analyze measurement errors

    Estimate amplitude error due to magnetizing current and phase shift from the interaction of burden resistor and magnetizing inductance over the operating frequency range. If needed, refine turns ratio or burden value to keep amplitude and phase errors within your design targets for current‑mode control or protection thresholds.

  5. Step 5: Validate with case study

    Add any required secondary diodes or clamps to ensure proper core reset and to protect the CST and controller inputs, then prototype the design in the actual SMPS or automotive converter. Measure sense waveforms, verify that current limits and protections behave as intended, and iterate component values only if necessary.

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