Replace Batteries in Power Ride-Through Applications with Robust Supercaps and 3mm × 3mm Capacitor Charger


Supercapacitors (or ultracapacitors) are finding their way into an increasing number of applications for short-term energy storage and applications that require intermittent high energy pulses. One such application is a power ride-through circuit, in which a backup energy source cuts in and powers the load if the main power supply fails for a short time. This type of application has been dominated by batteries in the past, but electric double layer capacitors (EDLCs) 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. Supercaps are switched into the power path when needed and the power to the load is controlled by a DC/DC converter. The LTC3225 supercapacitor charger has a number of features that make it a good choice for power ride-through applications. It comes in a small, 10-lead 3mm × 3mm DFN package and features programmable charging current, automatic cell voltage balancing, low drain current on the supercapacitors and a patent pending, low noise, constant current charger.

Supercapacitor Characteristics

Supercapacitors come in a variety of sizes, for example a 10F/2.7V supercap is available in a 10mm × 30mm 2-terminal radial can with an ESR of 25mΩ while a 350F/2.5V supercapacitor with an ESR of 1.6mΩ 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. Initial leakage current is a misnomer in that the initial leakage current is really dielectric absorption current which disappears after some time. 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 overcharging of one of the series capacitors. Passive cell balancing, where a resistor is placed across the capacitor, 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 2μA/Farad. Given these parameters, a 10F, 2.5V supercapacitor would require a 2.5k balancing resistor. This resistor would drain 1mA of current from the supercapacitor when the charging circuit is disabled.

An alternative is to use a non-dissipative active cell balancing circuit, such as the LTC3225, to maintain cell voltage. The LTC3225 presents less than 4μA of load to the supercapacitor when in shutdown mode and less than 1μA when input power is removed. The LTC3225 features a programmable charging current of up to 150mA, charging two series supercapacitors to either 4.8V or 5.3V 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 the minimum operating voltage, the worst case RT is

Equation 2

The voltage required across the supercapacitor at the undervoltage lockout 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 effective capacitance of a series connected bank of capacitors is the effective capacitance of a single capacitor divided by the number of capacitors while the total ESR is the sum of all the series ESRs.

The ESR of a supercapacitor decreases with higher frequency. Manufacturers usually specify the ESR at 1kHz, while some manufactures publish both the value at DC and at 1kHz. The capacitance of supercapacitors also decreases as frequency increases and is usually specified at DC. The capacitance at 1kHz is about 10% of the value 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 0.3Hz.


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

Figure 1. A 5V power ride-through application

Figure 2 shows a 12V power system that uses six 10F, 2.7V supercapacitors in series charged by three LTC3225’s set to 4.8V and a charging current of 150mA. The three LTC3225’s are powered by three floating 5V 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 1.8V at 11A from the OR’d outputs. The LTC4355’s MON1 in this application is set for 10.8V.

Figure 2. A 12V power ride-through application


Supercapacitors are meeting the needs of power ride-through applications where the time requirements are in the seconds to minutes range. Capacitors 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.


Jim Drew

Jim Drew。2007年アナログ・デバイセズに入社。同社ボストン(マサチューセッツ州)の設計センターでシニア・アプリケーション・エンジニアとして勤務。アプリケーション固有パワーICのアプリケーション・サポートを担当ソーラー電力、エナジー・ハーベスティング、スーパーキャパシタ・チャージャ・アクティブ・バッテリ・バランシングなどを対象とするパワー・コンディショニング・アプリケーションに関心を持つ。これまで、EMC、Hewlett Packard、Compaq、Digital Equipment Corporationでコンサルティング・エンジニアとして勤務、パワー・システムの開発に従事。また、2017年に退職後、マサチューセッツ大学ローウェル校電子工学科の非常勤講師として教鞭をとる。ローウェル工科大学(Lowell Technical Institute、現在はマサチューセッツ大学ローウェル校)でBSEEおよびMSEEの学位を取得。