Supercapacitors replace batteries in power ride-through applications using tiny charger IC

Supercapacitors are finding their way into an increasing number of applications for short-term energy storage. One such application is a power ride-through circuit, in which a backup energy source cuts in and powers the load when main power supply fails for a short time. This type of application has been dominated by batteries in the past, but supercapacitors are fast making inroads as their price-per-farad, size and effective series resistance per capacitance (ESR/C) continue to fall.

In a power ride-through application, series-stacked capacitors must be charged and cell voltage balanced. Supercapacitors are switched into the power path when needed and the power to the load is controlled by a DC/DC converter. Features that make a good choice for power ride-through applications include small package size, programmable charging current, automatic cell voltage balancing, and low drain current on the supercapacitors and a, low noise, constant current charger.

Supercapacitor characteristics
Supercapacitors come in a variety of sizes, for example a 10 F/2.7 V supercapacitor is available in a 10 × 30 mm, 2-terminal radial can with an ESR of 25 mΩ, while a 350 F/2.5 V supercapacitor with an ESR of 1.6 mΩ is available in a D-cell battery form factor.

One advantage supercapacitors offer over batteries is their long life. A capacitor's cycle life is quoted as greater than 500,000 cycles; batteries are specified for only a few hundred cycles. This makes the supercapacitor an ideal “set and forget” device, requiring little or no maintenance.

Two parameters of the supercapacitor that are critical to an application are cell voltage and initial leakage current. The manufacturers of supercapacitors rate their leakage current after 100 hours of applied voltage, while the initial leakage current in those first 100 hours may be as much as 50 times the specified leakage current.

The voltage across the capacitor has a significant effect on its operating life. When used in series, the supercapacitors must have balanced cell voltages to prevent over-charging of one of the series capacitors. Passive cell balancing is a popular and simple technique. The disadvantage of this technique is that the capacitor discharges through the balancing resistor when the charging circuit is disabled. The rule of thumb for this scheme is to set the balancing resistor to 50 times the worst case leakage current, estimated at 2 μA/F.

An alternative is to use a non-dissipative, active cell-balancing circuit, such as the LTC3225 IC, to maintain cell voltage. The LTC3225 presents less than 4 μA of load to the supercapacitor when in shutdown mode and less than 1 μA when input power is removed. It also features a programmable charging current of up to 150 mA, charging two series supercapacitors while balancing the voltage on the capacitors.

Power ride-through applications

To provide a constant voltage to the load, a DC/DC converter is required between the load and the supercapacitor. As the voltage across the supercapacitor decreases, the current drawn by the DC/DC converter increases to maintain constant power to the load. The DC/DC converter drops out of regulation when its input voltage reaches the minimum operating voltage (VUV ).

To estimate the requirements for the supercapacitor, the effective circuit resistance (RT ) needs to be determined. RT is the sum of the capacitors' ESRs and the circuit distribution resistances, Equation 1 .

Assuming 10% of the input power is lost in the effective circuit resistance when the DC/DC converter is at VUV , the worst-case RT is (Equation 2 ):

The voltage required across the Supercapacitor at VUV threshold of the DC/DC converter is (Equation 3 ):

The required effective capacitance can then be calculated based on the required ride-through time (TRT ), and the initial voltage on the capacitor (VC(0) ) and VC(UV) (Equation 4 ):

The ESR of a supercapacitor decreases with higher frequency. Manufacturers usually specify the ESR at 1 kHz, while some manufactures publish both the value at DC and at 1 kHz. The capacitance of supercapacitors also decreases as frequency increases and is usually specified at DC. When using a supercapacitor in a ride-through application where the power is being sourced for seconds to minutes, use the effective capacitance and ESR measurements at a low frequency, such as 0.3 Hz.


Figure 1 shows two series connected 10 F/2.7 V supercapacitors charged to 4.8 V that can hold up 20 W. The LTC3225 is used to charge the supercapacitors at 150 mA and maintain cell balancing, while the LTC4412 provides an automatic switchover function. The LTM4616 dual output switch mode μModule DC/DC converter generates the 1.8 V and 1.2 V outputs.

Figure 1: A 5V power ride-through application

(Click on image to enlarge)

Figure 2 shows a 12 V power system that uses six 10 F/2.7 V supercapacitors in series charged by three LTC3225s set to 4.8 V, and a charging current of 150 mA.

Figure 2: A 5V power ride-through application

(Click on image to enlarge)

The three LTC3225s are powered by three floating 5-V outputs generated by the LT1737 flyback controller. The output of the stack of six supercapacitors is set up in a diode-OR arrangement via the LTC4355 dual ideal-diode controller. The LTM4601A μModule DC/DC regulator produces 1.8 V at 11 A from the OR'd outputs. The LTC4355's MON1 in this application is set for 10.8 V.


Supercapacitors are meeting the needs of power ride-through applications where the time requirements are in the seconds to minutes range. Supercapacitors offer long life, low maintenance, light weight and environmentally friendly solutions when compared to batteries. To this end, the LTC3225 provides a compact, low noise solution to charging and cell balancing series connected supercapacitors.

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