Tiny Controller Makes It Easy to Charge Large Capacitors


Emergency warning beacons, inventory control scanners, professional photoflash and many other systems operate by delivering a pulse of energy to a transducer. This energy typically comes from a large capacitor that has been charged to some predetermined voltage.

The LT3750 is a current-mode flyback controller optimized for charging large value capacitors to a user selected target voltage. This target voltage is set by the turns ratio of the flyback transformer and just two resistors in a simple, low voltage network, so there is no need to connect components to the high voltage output. The charging current is set by an external sense resistor and is monitored on a cycle-by-cycle basis. The LT3750 is available in a space saving MSOP-10 package.

The device is compatible with a wide range of control circuitry, being equipped with a simple interface consisting of a CHARGE command input bit and an open drain DONE status flag. Both of these signals are compatible with most digital systems, yet tolerate voltages as high as 24V.

Simple 300V, 400μF Charger

Figure 1 shows the schematic of a LT3750 circuit that charges a 400μF capacitor to a target voltage of 300V. The 1:10 turns ratio of T1 and the R1, R2 resistors set the target voltage to 300V, while the R4 power resistor sets the peak charging primary current to 7.5A.

Figure 1. Simple circuit charges a 400μF capacitor.

Operating from a 12V power source, this circuit charges the 400μF capacitor to 300V in 1.04 seconds, as shown in Figure 2.

Figure 2. Output voltage and input current waveforms of LT3750 capacitive charging circuit.

Design Considerations

The architecture balances a high degree of integration with flexibility—leaving key parameters definable by the user. The important issues to consider in completing a design are input capacitor sizing, transformer design and output diode selection.

Power Stage Input Capacitor

Every switching cycle, the LT3750 measures the voltage at its RVOUT pin to determine the transformer, T1, flyback voltage. It also measures the signal at its VTRANS pin, which is the voltage at the input of the power switching stage. The difference of these two signals, accounting for the T1 transformer turns ratio and the D1 rectifying diode, yields the output voltage. In order to get an accurate result, it is important that the signal at the LT3750’s VTRANS input optimally reflects the DC potential of the power stage input. Consequently, the capacitance at the input of the power switching stage must be chosen such that the ripple voltage at the VTRANS input is not excessive. The capacitor bank in the circuit represented by Figure 1 is actually made of five capacitors. C1 is a single 150μF electrolytic capacitor to provide bulk energy, C2 is three low ESR 22μF ceramic capacitors to accommodate the high switching currents, and C3 is low ESR 10μF ceramic capacitor that provides local decoupling to the LT3750. For best results, place C1 and C2 as close as possible to T1, and C3 as close as possible to the VTRANS pin on the LT3750.


Other than the turns ratio, there are two issues to remember when selecting a transformer. The first is that the transformer secondary must be constructed to withstand potentials of both the positive and negative voltages associated with charging the capacitor. This withstand voltage is not the same as the isolation voltage rating. In the case of the circuit shown in Figure 1, there is no isolation voltage requirement, as the primary and secondary of T1 are tied to the same ground reference. The secondary winding, however, is subjected to the output potential, or 300V, and care must be taken in selecting for parameters relevant to such high voltages, such as pin spacing and wire insulation.

The other transformer parameter to keep in mind is the primary inductance. The primary inductance determines the operating frequency range, input current ripple and core loss, all of which contribute to the capacitor charge time and efficiency. The charging profile shown in Figure 2 is for a circuit using a transformer with a primary inductance of 10μH. Figure 3 shows the charging profile for the same circuit, but the primary inductance is much larger, 51μH. Note that the 51μH transformer has a longer charge time than the 10μH transformer.

Figure 3. A transformer with a 51μH primary inductance has a longer charge time and larger input current ripple than a transformer with a 10μH primary inductance.

Table 1 gives a summary of the input charging current and charge times for LT3750 circuits for three different T1 primary inductances, with the 15μH device giving the best result.

Table 1. Summary of input charging current and charge times for LT3750 circuits for transformers with different primary inductances
Transformer Primary Inductance Input Charging Current Input Charging Current Ripple Charge Time
TDK DCT20EFD-UXXS003 10μH 2.2A 0.5A 1040ms
Coiltronics CTX02-17314 15μH 2.2A 0.4A 1000ms
Coiltronics CTX02-17144 51μH 2A 1.4A 1120ms

Output Diode

Finally, it is important to consider the high AC voltages when selecting the output rectifying diode. The circuit in Figure 1 has a 300V output, but the output rectifying diode must withstand the sum of the output voltage and the voltage across the transformer secondary when the MOSFET Q1 is on. In this case, that is about 500V. This is a high voltage, but there are many manufacturers that produce switching diodes suitable for this application.

While it is important to minimize board space, the designer must choose a device that does not cause a violation of the spacing requirements for both safety and producibility. According to table 6-1, “Electrical Conductor Spacing,” of IPC-2221, Generic Standard on Printed Circuit Board Design (February 1998 release), the minimum spacing between conductors that have a potential up to 500V must be no less than 2.5mm on an uncoated printed circuit board operated below an altitude of 3050m. The output diode must be chosen to ensure that the minimum spacing between the diode pads is at least 2.5mm.

The circuit shown in Figure 1 uses a MURS160, which is offered by a number of manufacturers such as Diodes Inc and Vishay. It is an ultrafast recovery rectifier and has a peak repetitive reverse voltage rating of 600V. The diode comes in an SMB package, which allows the edge-to-edge separation between the pads to be as much as 3mm.

David Ng

David Ng

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