April 2011 I N T H I S I S S U E dual input/output 3A monolithic buck with 3V–36V input range 10 Volume 21 Number 1 Harvest Energy from a Single Photovoltaic Cell Nathan Bourgoine how to drive low power, 1Msps, 16-bit, differential input ADC from singleended signals 30 maximize output power from current-limited USB and PCMCIA sources 38 dual output step-down controller converts 60V directly to 3.3V 40 POWER SUPPLY CONNECTOR DROPS WIRING DROPS CONNECTOR DROPS WIRING DROPS To simplify the distribution of wireless communications for instrumentation, monitoring and control applications, power supply designers strive for device grid-independence. Batteries, the immediately obvious solution, offer the illusion of grid independence, but require replacement or recharging, which means eventual connection to the grid and expensive human intervention and maintenance. Enter energy harvesting, where energy is collected from the instrument’s immediate environment, offering perpetual operation with no connection to the grid and minimal or no maintenance requirements. CONNECTOR DROPS LOAD CONNECTOR DROPS Figure 1. The simplest model for load regulation over resistive interconnections. Caption A variety of ambient energy sources can be harvested to produce electrical power, including mechanical vibration, temperature differential and incident light. Linear Technology produces power management solutions that solve the problems specific to harvesting ambient low energy sources, including the LTC®3588 for vibration sources, the LTC3108/LTC3109 for thermal, and now the LTC3105 for photovoltaic energy harvesting applications. Photovoltaic energy harvesting is widely applicable, given that light is almost universally available, photovoltaic (PV) cells are relatively low cost and they produce relatively high power compared to other ambient energy harvesting solutions. Because of its relatively high energy output, photovoltaic energy harvesting can be used to power wireless sensor nodes, as well as higher power battery charging applications to extend battery life, in some cases eliminating tethered charging altogether. While high voltage stacks of series-connected photovoltaic cells are prolific, single PV-cell solutions are rare, due to the difficulty of generating useful power rails from the low voltage produced by a single PV cell under load. Few boost converters can produce outputs from a low voltage, relatively (continued on page 2) w w w. li n ea r.com …continued from the cover In this issue... COVER STORY Harvest Energy from a Single Photovoltaic Cell 1 DESIGN FEATURES Protect Mobile Devices from Hot Plug Transients (to 85V) and from Users Who Use the Wrong Power Adapter Kevin Wong (LTC3105, continued from page 1) 7 Monolithic, Dual 3A Input/Output Buck with 3V–36V Operating Range Simplifies and Shrinks DC/DC Converters in Automotive, Industrial and Distributed Power Applications Jonathan Paolucci 10 3A Output, 96% Efficient Buck-Boost DC/DC Converter Sets the Standard for Power Density and Noise Performance Richard Cook 19 22 Low IQ, Triple Output Boost/Buck/Buck Synchronous Controller Keeps Electronics Running Through Battery Transients in Automotive Start-Stop and Always-On Systems Joe Panganiban and Jason Leonard 26 DESIGN IDEAS How to Drive Low Power, 1Msps, ±2.5V Differential-Input, 16-Bit ADC with a Variety of Single-Ended Signals Guy Hoover 30 Easy, Isolated Low Power Telecom Supply: No Opto-Isolator Required Mayur Kenia 32 4mm × 5mm, Dual Input/Output, Synchronous Monolithic Buck Regulator Converts 12V to 1.2V at 4MHz Phil Juang Figure 1. Simple photovoltaic cell model Two common parameters that characterize a PV cell are the open circuit voltage and the short-circuit current. Typical curves for PV cell current and voltage are shown in Figure 2. Note that the short-circuit current is the output of the model’s current generator while the open circuit voltage is the forward voltage of the model’s diode. As light levels increase, the current from the generator increases and the IV curves move up. To extract maximum power from the PV cell, the input resistance of the power converter must be matched to the output resistance of the cell, resulting in operation at the maximum power point. Figure 3 shows the power curve for a typical single photovoltaic cell. To ensure maximum power extraction, the output voltage of the PV cell should be operated at the peak of the power curve. The LTC3105 adjusts the output current delivered to the load in order to maintain the PV cell Figure 2. Typical photovoltaic cell IV curve Figure 3. Typical photovoltaic cell power curve 34 250 36 Jason Leonard and Joe Panganiban 40 product briefs 43 back page circuits 44 90 80 BRIGHTER 200 OUTPUT CURRENT (mA) 38 Low IQ, Dual Output Step-Down Controller Converts 60V Directly to 3.3V 150 100 60 50 40 30 20 50 0 BRIGHTER 70 DIMMER 0 0.1 0.4 0.2 0.3 CELL VOLTAGE (V) 2 × 1 INCH POLYCRYSTALLINE CELL 2 | April 2011 : LT Journal of Analog Innovation – (continued on page 4) Buck-Boost Converter with Accurate Input Current Limit Maximizes Power Utilization from USB and PCMCIA Sources Michael Munroe VCELL Photovoltaic sources can be electrically modeled by a current source connected in parallel with a diode as shown in Figure 1. More complex models show secondary effects, but for our purposes this model is sufficient. Isolated Flyback Converters Eliminate Opto-Coupler Yat Tam + UNDERSTANDING PHOTOVOLTAIC CELL SOURCES Intermediate Bus Buck Regulator Maintains 5V Gate Drive During Automobile Cold Crank Conditions Theo Phillips and Tick Houk high impedance single PV cell. The LTC3105, however, is designed specifically to meet these challenges. Its ultralow 250mV start-up voltage and programmable maximum power point control allow it to generate the typical voltage rails (1.8V–5V) required for most applications from challenging PV sources. POWER (mW) Nathan Bourgoine The LTC3105 enables autonomous remote sensor nodes, data collection systems and other applications that require grid independence and minimal maintenance. DIMMER 10 0.5 0.6 0 0 0.1 0.4 0.2 0.3 CELL VOLTAGE (V) 2 × 1 INCH POLYCRYSTALLINE CELL 0.5 0.6 While high voltage stacks of series-connected photovoltaic cells are prolific, single PV-cell solutions are rare, due to the difficulty of generating useful power rails from the low voltage produced by a single PV cell under load. 90 (LTC3105, continued from page 2) LTC3105 voltage at the voltage set by the maximum power point control pin. Therefore, a single programming resistor establishes the maximum power point and ensures maximum power extraction from the PV cell and peak output charging current. 10µA VIN RMPPC + – –g m + 60 50 40 MPPC VOLTAGE 30 20 DIMMER 10 0 0 0.1 0.4 0.2 0.3 CELL VOLTAGE (V) 0.5 0.6 2 × 1 INCH POLYCRYSTALLINE CELL Figure 4. Maximum power point control mechanism Figure 5. Err on the side of a lower voltage when choosing a maximum power point voltage to avoid the steep drop-off inches is sufficient to run many remote sensors and to trickle charge a battery. presents design challenges. Even a large high efficiency crystalline cell with an area of four square inches generates only 860µW in typical office lighting. In contrast, devices operating from indoor lighting have far less energy available to them. Common indoor lighting is roughly 0.25% as strong as full sunlight (the huge difference in intensity between indoor lighting and sunlight is hard to perceive due to the human eye’s ability to adjust to a wide range of illumination levels). The dramatically lower light levels available to indoor applications Figure 6. Li-ion charging circuit L1 10µH 225mV TO 500mV L1: COILCRAFT MSS5131-103MX VIN + SW VOUT 4.1V VOUT 10µF LTC3105 1020k FB OFF ON 40.2k LDO SHDN AUX 1µF Li-ION PGOOD MPPC 4 | April 2011 : LT Journal of Analog Innovation POWER (mW) MPPC The amount of power that can be generated using a photovoltaic cell depends on a number of factors. The output power of the cell is proportional to the brightness of the light landing on the cell, the total area of the cell, and the efficiency of the cell. Most PV cells are rated for use under full direct sunlight (1000W/m2), but such ideal conditions are unlikely to occur in most applications. For devices operating from sunlight, the peak power available from the cell can easily change by a factor of ten from day to day due to weather, season, haze, dust, and incident angle of the sunlight. Typical output power for a crystalline cell in full sunlight is about 40mW per square inch depending on cell characteristics. A PV cell with an area of a few square – IPEAK VCC BRIGHTER 70 BOOST CONVERTER HOW MUCH POWER IS AVAILABLE? PHOTOVOLTAIC CELL 80 332k 2.2V FBLDO GND 4.7µF 10µF CHOOSING THE MAXIMUM POWER POINT CONTROL VOLTAGE Figure 4 shows a model of the maximum power point control mechanism used by the LTC3105. Figure 3 shows the power curve for a PV cell. Note that PV cell power declines sharply from its peak as the cell voltage rises away from peak power. It is thus generally more desirable to err on the side of a lowerthan-ideal control voltage, rather than a higher voltage, because the power curve rolls off more sharply on the high side. When selecting the MPPC tracking voltage, various operating conditions must be considered. Typically, the maximum power point does not move substantially with changes in illumination. As a result, it is design features The LTC3105’s integrated maximum power point control and low voltage start-up functionality enable direct operation from a single PV cell and ensure optimal energy extraction. The LTC3105 can be used to directly power circuitry or for charging energy storage devices to allow operation through dark or low light periods. 11 SUNNY DAY OUTPUT CURRENT (mA) 9 BUILDING SHADOW 7 5 3 1 –1 7:00 RAINY OVERCAST DAY 10:00 13:00 16:00 TIME OF DAY 19:00 2 × 1 INCH POLYCRYSTALLINE CELL Figure 7. Charging profiles for two square inch photovoltaic cell possible to choose a single tracking voltage that provides operation near the maximum power point for a wide range of illumination levels. Even though the operating point will not be precisely at the maximum power point at extreme levels of illumination, the reduction in output power from the ideal is usually only 5%–10%. For the power curve shown in Figure 5, an MPPC voltage of 0.4V yields performance near the maximum power point at either illumination extreme. The voltage difference from the maximum power point is approximately 20mV in both cases, resulting in a power loss of less than 3%. As a rule of thumb, the maximum power point control voltage should be around 75%–80% of the open circuit voltage for the PV cell. Tracking the cell to this voltage results in a cell output current that is 75%–80% of the short-circuit current. LI-ION BATTERY CHARGING IN OUTDOOR LIGHTING CHOOSING THE RIGHT ENERGY STORAGE DEVICE One of the challenges faced by applications using a photovoltaic source is the lack of input power during darkness and low light conditions. For most applications this necessitates use of energy storage elements such as a supercapacitor or rechargeable battery that is large enough to provide power throughout the longest expected dark period. There are many alternatives for storing harvested energy, including a wide variety of rechargeable battery technologies and high energy density capacitors. No one technology is perfect for all applications. When selecting the storage element for your application, consider a number of factors, including the self-discharge rate, maximum charge and discharge current, voltage sensitivity, and cycle lifetime. Figure 7 shows the measured charging current profile using a 2” × 1” polycrystalline PV cell to charge a Li-ion battery using the LTC3105 circuit shown in Figure 6. The upper curve of Figure 7 shows the charging current on a typical clear day with full sun. The lower curve shows the charging current observed over the course of a heavily overcast day. Even under these low light conditions a charging current of 250µ A or more was maintained throughout the day totaling 6mAh of charge delivered to the battery. The self-discharge rate is particularly important in photovoltaic applications. Given the limited amount of charging current available in most photovoltaic power applications, a high self-discharge rate may consume a large portion of the available energy from the PV source. Some energy storage elements, such as large supercapacitors, may have self-discharge current in excess of 100µ A, which could dramatically reduce the net charge accumulated over a daily charge cycle. Figure 8. A Li-ion trickle charger operates from a single photovoltaic cell L1 10µH 225mV TO 500mV PHOTOVOLTAIC CELL L1: COILCRAFT MSS5131-103MX VIN + SW 10µF – VOUT VOUT LTC3105 1020k ADJ FB PGOOD MPPC OFF ON 40.2k LDO SHDN AUX 1µF 2.2V FBLDO GND NTC 332k 10µF BAT Li-ION LBSEL 4.7µF VCC LTC4071 GND April 2011 : LT Journal of Analog Innovation | 5 The LTC3105 is a complete single-chip solution for energy harvesting from low cost, single photovoltaic cells. Another key consideration is the rate at which the energy storage device can be charged. For example, a lithium coin cell with a maximum charging current of 300µ A requires a large resistor between it and the output of the LTC3105 in order to prevent overcurrent conditions. This can put a limit on the amount of energy harvested, decreasing the amount of energy available to the application. In many cases the charge rate is proportional to another important factor, cycle lifetime. The cycle life of a storage element determines how long it can operate in the field without maintenance. Generally, faster charging and discharging reduces the operational life of the element. Supercapacitors offer very good cycle life, while batteries charged with relatively high currents (charge > 1C) have degraded lifetimes. In addition to the charge and discharge rate, the depth – VIN SW VOUT CIN 10µF – FB OFF ON MPPC PGOOD SHDN LDO CAUX 1µF AUX RMPPC 40.2k of each charge/discharge cycle can affect the lifetime of batteries, with deeper cycles leading to shorter life times. With several battery types, notably lithium and thin film, the maximum and minimum voltage must be carefully controlled. The VOUT 3.3V COUT 100µF R2 1.02M XMTR I/O OFF ON EN PGOOD SHDN LDO AUX CAUX 1µF 2.2V FBLDO GND * COILCRAFT MSS5131-103MX 6 | April 2011 : LT Journal of Analog Innovation + NiMH ×2 1.8V FBLDO GND COUT 10µF VOUT 3.2V + R4 1.27M CLDO 4.7µF Figure 9. Single-cell photovoltaic NiMH trickle charger R1 2.32M FB R2 470k R3 1M RMPPC 40.2k VOUT LTC3105 R1 1.02M LTC3105 SW CIN 10µF MPPC 2N7000 VIN + Figure 10. Single-cell-powered remote wireless sensor L1* 10µH + L1, 10µH µC RPG 499k VDD CLDO 4.7µF A/D GPIO GND SENSOR maximum charge voltage is well controlled in LTC3105 applications since the converter terminates charging when the output comes into regulation. To prevent over-discharge, the LTC3105 can be used in conjunction with the LTC4071 shunt battery charger as shown in Figure 8. CONCLUSION The LTC3105 is a complete single chip solution for energy harvesting from low cost, single photovoltaic cells. Its integrated maximum power point control and low voltage start-up functionality enable direct operation from a single PV cell and ensure optimal energy extraction. The LTC3105 can be used to directly power circuitry or for charging energy storage devices to allow operation through dark or low light periods. The LTC3105 makes it possible to produce autonomous remote sensor nodes, data collection systems and other applications that require grid independence and minimal maintenance. n