MIC2208 3mm x 3mm 1MHz 3A PWM Buck Regulator General Description Features The Micrel MIC2208 is a high efficiency PWM buck (stepdown) regulator that provides up to 3A of output current. The MIC2208 operates at 1MHz and has external compensation that allows a closed loop bandwidth of over 100kHz. The low on-resistance internal p-channel MOSFET of the MIC2208 allows efficiencies over 94% reduces external component count and eliminates the need for an expensive current sense resistor. The MIC2208 operates from 2.7V to 5.5V input and the output can be adjusted down to 1V. The devices can operate with a maximum duty cycle of 100% for use in lowdropout conditions. The MIC2208 is available in the exposed pad 12-pin 3mm x 3mm MLF(R) package with a junction operating range from -40C to +125C. Datasheets and support documentation can be found on Micrel's web site at: www.micrel.com. * * * * * * * * * * * * * 2.7 to 5.5V supply voltage 1MHz PWM mode Output current to 3A >90% efficiency Adjustable output voltage option down to 1V Ultra-fast transient response External Compensation Stable with a wide range of output capacitance Fully integrated 5A MOSFET switch Micropower shutdown Thermal shutdown and current limit protection Pb-free 12-pin 3mm x 3mm MLF(R) package -40C to +125C junction temperature range Applications * * * * * 5V or 3.3V Point of Load Conversion Telecom/Networking Equipment Set Top Boxes Storage Equipment Video Cards ___________________________________________________________________________________________________________ Typical Application MIC2208 3A 1MHz Buck Regulator MLF and MicroLeadFrame are registered trademarks of Amkor Technology, Inc. Micrel Inc. * 2180 Fortune Drive * San Jose, CA 95131 * USA * tel +1 (408) 944-0800 * fax + 1 (408) 474-1000 * http://www.micrel.com September 2007 M9999-090707-C Micrel, Inc. MIC2208 Ordering Information Part Number Voltage Temperature Range Package Lead Finish MIC2208YML Adj. -40 to +125C 12-Pin 3x3 MLF(R) Pb-Free Note: (R) MLF is GREEN RoHS compliant package. Lead finish is NiPdAu. Mold compound is Halogen Free. Pin Configuration SW 1 12 SW VIN 2 11 VIN PGND 3 10 PGND SGND 4 9 PGOOD BIAS 5 FB 6 8 EN EP 7 COMP 12-Pin 3mm x 3mm MLF(R) (ML) Pin Description Pin Number Pin Name Pin Function 1, 12 SW Switch (Output): Internal power P-Channel MOSFET output switch. 2, 11 VIN Supply Voltage (Input): Supply voltage for the source of the internal P-channel MOSFET and driver. Requires bypass capacitor to GND 3, 10 PGND Power Ground. Provides the ground return path for the high-side drive current. 4 SGND Signal Ground. Provides return path for control circuitry and internal reference. 5 BIAS Internal circuit bias supply. Must be bypassed with a 0.1F ceramic capacitor to SGND. 6 FB 7 COMP 8 EN 9 PGOOD EP GND September 2007 Feedback. Input to the error amplifier, connect to the external resistor divider network to set the output voltage. Compensation. This is the internal error amplifier output. Connect external compensation components for type II or type III compensation. Enable (Input). Logic level low will shutdown the device, reducing the current draw to less than 5A. Power Good. Open drain output that is pulled to ground when the output voltage is within 7.5% of the set regulation voltage Connect to ground. 2 M9999-090707-C Micrel, Inc. MIC2208 Absolute Maximum Ratings(1) Operating Ratings(2) Supply Voltage (VIN) ........................................ -0.3V to +6V Output Switch Voltage (VSW) .............................. -1V to +6V Output Switch Current (ISW)............................................10A Logic Input Voltage (VEN) .................................. -0.3V to VIN Storage Temperature (Ts) ........................... -60C to 150C ESD Rating(3) .......................................................2kV (HBM) Supply Voltage (VIN)..................................... +2.7V to +5.5V Logic Input Voltage (VEN, VLOWQ)............................ 0V to VIN Junction Temperature (TJ) ........................ -40C to +125C Junction Thermal Resistance 3x3 MLF-12 (JA) ...............................................60C/W Electrical Characteristics(4) VIN = VEN = 3.6V; L = 1H; COUT = 4.7F; TA = 25C, unless noted. Bold values indicate -40C< TJ < +125C. Parameter Condition Min (turn-on) 2.45 Supply Voltage Range Under-Voltage Lockout Threshold Typ Max Units 5.5 V 2.55 2.65 V 2.7 UVLO Hysteresis 100 mV Quiescent Current VFB = 0.9 * VNOM (not switching) 720 950 Shutdown Current VEN = 0V 0.1 5 A [Adjustable] Feedback Voltage 1% 2% (over temperature) 1 1.01 1.02 V V 1 100 nA 8 10 A 0.99 0.98 FB pin input current A Current Limit in PWM Mode VFB = 0.9 * VNOM Output Voltage Line Regulation VOUT > 2.2V; VIN = VOUT + 500mV to 5.5V; ILOAD = 20mA VOUT < 2.2V; VIN = 2.7V to 5.5V; ILOAD = 20mA 0.13 Output Voltage Load Regulation 20mA < ILOAD < 3A 0.2 1 % PWM Switch ONResistance ISW = 50mA VFB = 0.7VFB_NOM (High Side Switch) 95 20 300 m m % Oscillator Frequency 0.9 1 1.1 MHz Enable Threshold 0.5 0.85 1.3 V 0.1 2 A Enable Input Current Soft Start Time 450 s Over-Temperature Shutdown 160 C over-Temperature Hysteresis 20 C Power Good Range 7 10 % 145 200 Power Good Resistance VOUT =10% to VOUT = 90% IPGOOD Notes: 1. Exceeding the absolute maximum rating may damage the device. 2. The device is not guaranteed to function outside its operating rating. 3. Devices are ESD sensitive. Handling precautions recommended. Human body model, 1.5k in series with 100pF. 4. Specification for packaged product only. September 2007 3 M9999-090707-C Micrel, Inc. MIC2208 Typical Characteristics 3.3V 96 MIC2208 Efficiency OUT 4.5VIN EFFICIENCY (%) 94 92 90 5VIN 5.5VIN 88 86 84 82 1.2V 85 75 73 71 69 67 1.0100 1.008 1.006 1.004 1.002 1.0080 1.0060 OUTPUT VOLTAGE (V) September 2007 EFFICIENCY (%) Feedback Voltage vs. Temperature 1.20 5.5VIN 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) 3 Feedback Voltage vs. Temperature 1.10 1.05 1.0020 1.0000 1.00 0.9980 0.95 0.9960 0.9940 3 5VIN 1.15 1.0040 0.90 0.9920 3.3V IN 0.9900 -40 1.000 0.998 0.996 0.994 0.992 3.3V IN 0.990 0 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) 65 0 3 FEEDBACK VOLTAGE (V) 1.010 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) 75 73 71 69 67 TEMPERATURE (C) 4 0.85 3.3V IN 0.80 120 Load Regulation 3.6VIN 4.5VIN 80 65 0 3 3.3VIN 83 81 79 77 MIC2208 Efficiency 100 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) 85 3VIN 3 OUT 60 65 0 1.2V OUT 40 IN 75 73 71 69 67 MIC2208 Efficiency 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) 0 5.5V 83 81 79 77 3.6VIN 75 70 0 3 3.3VIN 20 OUT 80 -20 MIC2208 Efficiency 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) EFFICIENCY (%) 3 3VIN 85 -40 72 70 0 4.5VIN 5VIN 78 76 74 MIC2208 Efficiency OUT FEEDBACK VOLTAGE (V) EFFICIENCY (%) 85 5VIN 90 120 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) 1.5V 83 81 79 77 3.6VIN 84 82 80 95 80 IN 1.5V 100 3.3V 4.5VIN 60 77 75 0 IN 90 88 86 40 83 81 79 3V MIC2208 Efficiency OUT 20 89 87 85 1.8V EFFICIENCY (%) EFFICIENCY (%) 95 93 91 MIC2208 Efficiency OUT 0 1.8V 3 -20 0.5 1 1.5 2 2.5 OUTPUT CURRENT (A) EFFICIENCY (%) 80 0 TEMPERATURE (C) M9999-090707-C Micrel, Inc. MIC2208 Typical Characteristics (continued) 300 200 100 1 0.8 0.6 0.6 0.4 0.4 0 2.7 120 80 100 60 40 0 20 -20 -40 0.2 0.2 3.3VIN TEMPERATURE (C) Max. Continuous Current vs. Ambient Temp 3.3V * *Using recommended layout (1oz copper) and B.O.M. 3 2.5 OUT 3.5 *Using recommended layout (1oz copper) and B.O.M. 3 2.5 2 1.5 2 5VIN 0 60 70 80 90 100 110 120 AMBIENT TEMPERATURE (C) 5VIN 3.3VIN 1.5 1 TEMPERATURE (C) Max. Continuous Current vs. Ambient Temp 2.5V * MAX. OUTPUT CURRENT (A) OUT 3.5 0 3.2 3.7 4.2 4.7 SUPPLY VOLTAGE (V) Max. Continuous Current vs. Ambient Temp 1.8V * OUT 3.5 3 2.5 2 3.3VIN 1.5 1 0.5 120 20 100 40 80 60 1 60 80 Enable Threshold vs. Temperature 1.2 0.8 100 3.2 3.7 4.2 4.7 5.2 SUPPLY VOLTAGE (V) 40 ENABLE THRESHOLD (V) 120 MAX. OUTPUT CURRENT (A) Enable Threshold vs. Supply Voltage 1.2 140 70 2.7 1 2 3 4 5 SUPPLY VOLTAGE (V) 0 RDSON vs. Temperature 160 P-CHANNEL RDSON (mOhms) 0 0 1 2 3 4 5 SUPPLY VOLTAGE (V) ENABLE THRESHOLD (V) 0 0 20 0.2 85 80 75 -20 0.4 0.5 100 95 90 400 0.6 -40 FEEDBACK VOLTAGE (V) 500 0.8 0 115 110 105 600 1.0 RDSON vs. Supply Voltage 120 P-CHANNEL RDSON (mOhms) 700 QUIESCENT CURRENT (A) 1.2 Quiescent Current vs. Supply Voltage MAX. OUTPUT CURRENT (A) Feedback Voltage vs. Supply Voltage 5VIN 1 *Using recommended 0.5 layout (1oz copper) 0 60 70 80 90 100 110 120 AMBIENT TEMPERATURE (C) and B.O.M. 0 60 70 80 90 100 110 120 AMBIENT TEMPERATURE (C) Max. Continuous Current vs. Ambient Temp 1.0V * OUT MAX. OUTPUT CURRENT (A) 3.5 3 2.5 2 5VIN 3.3VIN 1.5 1 *Using recommended 0.5 layout (1oz copper) September 2007 and B.O.M. 0 60 70 80 90 100 110 120 AMBIENT TEMPERATURE (C) 5 M9999-090707-C Micrel, Inc. MIC2208 Functional Characteristics September 2007 6 M9999-090707-C Micrel, Inc. MIC2208 Functional Diagram VIN VIN P-Channel Current Limit BIAS HSD SW SW PWM Control EN Enable and Control Logic COMP Bias, UVLO, Thermal Shutdown Soft Start EA FB 1.0V PGOOD 1.0V SGND PGND MIC2208 Block Diagram September 2007 7 M9999-090707-C Micrel, Inc. MIC2208 Pin Description VIN Two pins for VIN provide power to the source of the internal P-channel MOSFET along with the current limiting sensing. The VIN operating voltage range is from 2.7V to 5.5V. Due to the high switching speeds, a 10F capacitor is recommended close to VIN and the power ground (PGND) for each pin for bypassing. Please refer to layout recommendations. SW The switch (SW) pin connects directly to the inductor and provides the switching current necessary to operate in PWM mode. Due to the high speed switching on this pin, the switch node should be routed away from sensitive nodes. This pin also connects to the cathode of the free-wheeling diode. PGOOD Power good is an open drain pull down that indicates when the output voltage has reached regulation. For a power good low, the output voltage is within 10% of the set regulation voltage. For output voltages greater or less than 10%, the PGOOD pin is high. This should be connected to the input supply through a pull up resistor. A delay can be added by placing a capacitor from PGOOD to ground. BIAS The bias (BIAS) provides power to the internal reference and control sections of the MIC2208. A 10 resistor from VIN to BIAS and a 0.1F from BIAS to SGND is required for clean operation. EN The enable pin provides a logic level control of the output. In the off state, supply current of the device is greatly reduced (typically <1A). Do not drive the enable pin above the supply voltage. PGND Power ground (PGND) is the ground path for the MOSFET drive current. The current loop for the power ground should be as small as possible and separate from the Analog ground (AGND) loop. Refer to the layout considerations fro more details. FB The feedback pin (FB) provides the control path to control the output. For adjustable versions, a resistor divider connecting the feedback to the output is used to adjust the desired output voltage. The output voltage is calculated as follows: SGND Signal ground (SGND) is the ground path for the biasing and control circuitry. The current loop for the signal ground should be separate from the power ground (PGND) loop. Refer to the layout considerations for more details. R1 VOUT = VREF x + 1 R2 where VREF is equal to 1.0V. COMP The COMP pin is the output of the internal error amplifier. This pin is used to compensate the MIC2208 for stability over a varying range of external components. Refer to the compensation section of the datasheet for determining necessary component values. September 2007 8 M9999-090707-C Micrel, Inc. MIC2208 The output voltage is regulated by pulse width modulating (PWM) the switch voltage to the average required output voltage. The switching can be broken up into two cycles; On and Off. During the on-time, the high side switch is turned on, current flows from the input supply through the inductor and to the output. The inductor current is Application Information The MIC2208 is a 3A PWM non-synchronous buck regulator. By switching an input voltage supply, and filtering the switched voltage through an Inductor and capacitor, a regulated DC voltage is obtained. Figure 1 shows a simplified example of a non-synchronous buck converter. Figure 1. For a non-synchronous buck converter, there are two modes of operation; continuous and discontinuous. Continuous or discontinuous refer to the inductor current. If current is continuously flowing through the inductor throughout the switching cycle, it is in continuous operation. If the inductor current drops to zero during the off time, it is in discontinuous operation. Critically continuous is the point where any decrease in output current will cause it to enter discontinuous operation. The critically continuous load current can be calculated as follows: Figure 3. On-Time charged at the rate: (VIN - VOUT ) V VOUT - OUT VIN IOUT = 1MHz x 2 x L Continuous or discontinuous operation determines how we calculate peak inductor current. 2 L To determine the total on-time, or time at which the inductor charges, the duty cycle needs to be calculated. The duty cycle can be calculated as: D= Continuous Operation Figure 2 illustrates the switch voltage and inductor current during continuous operation. VOUT VIN and the On time is: D 1MHz Therefore, peak to peak ripple current is: TON = (VIN - VOUT ) x VOUT IPK -PK = 1MHz x L Figure 4 demonstrates the off-time. During the offtime, the high-side internal P-channel MOSFET turns off. Since the current in the inductor has to discharge, the current flows through the free-wheeling Schottky diode to the output. In this case, the inductor discharge rate is Figure 2. Continuous Operation September 2007 VIN 9 M9999-090707-C Micrel, Inc. MIC2208 (where VD is the diode forward voltage): TOFF = When the inductor current (IL) has completely discharged, the voltage on the switch node rings at the frequency determined by the parasitic capacitance and the inductor value. In Figure 5, it is drawn as a DC voltage, but to see actual operation (with ringing and all) refer to the functional characteristics. Discontinuous mode of operation has the advantage over full PWM in that at light loads, the MIC2208 will skip pulses as necessary, reducing gate drive losses, drastically improving light load efficiency. 1- D 1MHz Efficiency Considerations Calculating the efficiency is as simple as measuring power out and dividing it by the power in: Efficiency = Where input power (PIN) is: PIN = VIN x IIN and output power (POUT) is calculated as: POUT = VOUT x IOUT The Efficiency of the MIC2208 is determined by several factors. * RDSON (Internal P-channel Resistance) * Diode conduction losses * Inductor Conduction losses * Switching losses RDSON losses are caused by the current flowing through the high side P-channel MOSFET. The amount of power loss can be approximated by: PSW = RDSON x IOUT2 x D where D is the duty cycle. Since the MIC2208 uses an internal P-channel MOSFET, RDSON losses are inversely proportional to supply voltage. Higher supply voltage yields a higher gate to source voltage, reducing the RDSON, reducing the MOSFET conduction losses. A graph showing typical RDSON vs. input supply voltage can be found in the typical characteristics section of this datasheet. Diode conduction losses occur due to the forward voltage drop (VF) and the output current. Diode power losses can be approximated as follows: PD = VF x IOUT x (1-D) For this reason, the Schottky diode is the rectifier of choice. Using the lowest forward voltage drop will help reduce diode conduction losses, and improve efficiency. Duty cycle, or the ratio of output voltage-to-input voltage, determines whether the dominant factor in conduction losses will be the internal MOSFET or the Schottky diode. Higher duty cycles place the power losses on the high side switch, and lower duty cycles place the power losses on the schottky diode. Inductor conduction losses Figure 4. Off-Time Discontinuous Operation Discontinuous operation is when the inductor current discharges to zero during the off cycle. Figure 5 demonstrates the switch voltage and inductor currents during discontinuous operation. Figure 5. Discontinuous Operation September 2007 POUT x 100 PIN 10 M9999-090707-C Micrel, Inc. MIC2208 (PL) can be calculated by multiplying the DC resistance (DCR) times the square of the output current: PL = DCR x IOUT2 Also, be aware that there are additional core losses associated with switching current in an inductor. Since most inductor manufacturers do not give data on the type of material used, approximating core losses becomes very difficult, so verify inductor temperature rise. Switching losses occur twice each cycle, when the switch turns on and when the switch turns off. This is caused by a non-ideal world where switching transitions are not instantaneous, and neither are currents. Figure 6 demonstrates (Or exaggerates.) how switching losses due to the transitions dissipate power in the switch. Normally, when the switch is on, the voltage across the switch is low (virtually zero) and the current through the switch is high. This equates to low power dissipation. When the switch is off, voltage across the switch is high and the current is zero, again with power dissipation being low. During the transitions, the voltage across the switch (VS-D) and the current through the switch (IS-D) are at middle, causing the transition to be the highest instantaneous power point. During continuous mode, these losses are the highest. Also, with higher load currents, these losses are higher. For discontinuous operation, the transition losses only occur during the "off" transition since the "on" transitions there is no current flow through the inductor. Figure 6. Switching Transition Losses September 2007 11 M9999-090707-C Micrel, Inc. MIC2208 resistance for the FB resistors is very wide, R1 is recommended to be 10K. This minimizes the effect the parasitic capacitance of the FB node. Component Selection Input Capacitor A 10F ceramic is recommended on each VIN pin for bypassing. X5R or X7R dielectrics are recommended for the input capacitor. Y5V dielectrics lose most of their capacitance over temperature and are therefore, not recommended. Also, tantalum and electrolytic capacitors alone are not recommended due their reduced RMS current handling, reliability, and ESR increases. An additional 0.1F is recommended close to the VIN and PGND pins for high frequency filtering. Smaller case size capacitors are recommended due to their lower ESR and ESL. Please refer to layout recommendations for proper layout of the input capacitor. Bias filter A small 10 resistor is recommended from the input supply to the bias pin along with a small 0.1F ceramic capacitor from bias-to-ground. This will bypass the high frequency noise generated by the violent switching of high currents from reaching the internal reference and control circuitry. Tantalum and electrolytic capacitors are not recommended for the bias, these types of capacitors lose their ability to filter at high frequencies. Dominant Pole Gain (dB) Inductor Selection The MIC2208 is designed for use with a 1H inductor. Proper selection should ensure the inductor can handle the maximum average and peak currents required by the load. Maximum current ratings of the inductor are generally given in two methods; permissible DC current and saturation current. Permissible DC current can be rated either for a 40C temperature rise or a 10% to 20% loss in inductance. Ensure the inductor selected can handle the maximum operating current. When saturation current is specified, make sure that there is enough margin that the peak current will not saturate the inductor. Diode Selection Since the MIC2208 is non-synchronous, a free-wheeling diode is required for proper operation. A schottky diode is recommended due to the low forward voltage drop and their fast reverse recovery time. The diode should be rated to be able to handle the average output current. Also, the reverse voltage rating of the diode should exceed the maximum input voltage. The lower the forward voltage drop of the diode the better the efficiency. Please refer to the layout recommendations to minimize switching noise. 20dB/Decade LC Frequency Compensation The MIC2208 utilizes voltage mode compensation and has the error amplifier pin (COMP) pinned out to allow it to be compensated using external components. This allows the MIC2208 to be stable with a wide range of inductor and capacitor values. TYPE II compensation Type II compensation can be expressed as pole-zeropole. In our case, a dominant pole (R1 and C3) followed by a zero (C3 and R4), allowing the final pole to be provided by the output inductor and output capacitor (L and COUT). This mode of compensation works well when using higher ESR output capacitors, such as tantalum and electrolytic dielectrics. The ESR of the capacitor, along with the output capacitance provides a zero (COUT and ESR) that negates one of the two poles created by the inductor-output capacitor filter. This allows the gain to cross the 0dB point with a -1 slope (-20dB/decade). Feedback Resistors The feedback resistor set the output voltage by dividing down the output and sending it to the feedback pin. The feedback voltage is 1.0V. Calculating the set output voltage is as follows: R1 VOUT = VFB + 1 R2 Where R1 is the resistor from VOUT to FB and R2 is the resistor from FB to GND. The recommended feedback resistor values for common output voltages is available in the bill of materials on page x. Although the range of September 2007 Zero 12 M9999-090707-C Micrel, Inc. MIC2208 Type II Compensation 80 288 VIN=5VIN 70 VOUT=1.0V IOUT=3A Gain (dB) 60 252 216 50 180 40 144 30 108 20 72 10 36 0 0 -10 MIC2208 -36 -20 100 1k 10k 100k Frequency (KHz) -72 1M Bill of Materials Item Part Number C2012JB0J106K C1a, C1b GRM219R60J106KE19 Manufacturer TDK Description Qty. 10F Ceramic Capacitor X5R 0805 6.3V 2 (1) Murata(2) (3) 08056D106MAT AVX C2 0402ZD104MAT AVX(3) 0.1F Ceramic Capacitor X5R 0402 10V 1 C3 0402ZD100MAT AVX(3) 100pF Ceramic Capacitor X5R 0402 10V 1 470F Tantalum Capacitor 10V 1 3A Schottky 30V SMA 1 C4 TPME477M010R0030 D1 SSA33L RLF7030-1R0N6R4 L1 744 778 9001 IHLP2525AH-01 1 R1 R2 (3) AVX (4) Vishay Semi TDK (1) 1H Inductor 8.8m 7.1mm(L) x 6.8mm (W)x 3.2mm(H) Wurth Elektronik(5) (4) Vishay Dale 1H Inductor 12m 7.3mm(L)x7.3mm(W)x3.2mm(H) 1H Inductor 17.5m (L)6.47mmx(W)6.86mmx(H) 1.8mm (4) CRCW04023012F Vishay Dale CRCW04022002F Vishay Dale(4) 20 k 1% 0402 CRCW04023742F Vishay Dale(4) 37.4 k 1% 0402 For 1.8 VOUT CRCW04026042F (4) CRCW04021503F 30.1K 1% 0402 Resistor Vishay Dale 60.4 k 1% 0402 For 1.5 VOUT 150 k 1% 0402 For 1.2 VOUT (4) Open For 1.0 VOUT Vishay Dale CRCW04024993F (4) Vishay Dale 499K 1% 0402 Resistor (4) 1 For 2.5VOUT (4) Vishay Dale R4 1 1 1 R5 CRCW040210R0F Vishay Dale 10 1% 0402 Resistor 1 R6 CRCW04021002F Vishay Dale(4) 10K 1% 0402 Resistor 1 U1 MIC2208BML Micrel, Inc.(6) 1MHz 3A Buck Regulator 1 Notes: 1. TDK: www.tdk.com 2. Murata: www.murata.com 3. AVX: www.avx.com 4. Vishay: www.vishay.com 5. Wurth Elektronik Midcom, Inc.: www.midcom-inc..com 6. Micrel, Inc.: www.micrel.com September 2007 13 M9999-090707-C Micrel, Inc. MIC2208 Type III Open Loop Gain Response TYPE III compensation Type III in our case, is a dominant pole (C3 and R1) followed by a zero (C3 and R4) and an additional zero (C5 and R4), allowing the final pole to be provided by the output inductor and output capacitor. This mode of compensation is required when using low ESR output capacitors, such as ceramic capacitors. The additional zero offsets the double pole created by the inductor/output capacitor filter. Dominant Pole LC Frequency Gain(dB) Zero Zero 20dB/Decade Frequency (Hz) Type III Compensation 288 80 V IN=5V IN V OUT=1.0V IOUT=3A COUT=47F 70 Gain (dB) 60 252 216 50 180 40 144 30 108 20 72 MIC2208 36 10 Gain 0 Phase -36 -10 -20 100 1k 10k 100k -72 1M Frequency (KHz) Bill of Materials Item C1a, C1b Part Number Manufacturer C2012JB0J106K TDK(1) GRM219R60J106KE19 Murata(2) Description Qty. 10F Ceramic Capacitor X5R 0805 6.3V 2 (3) 08056D106MAT AVX C2 0402ZD104MAT AVX(3) 0.1F Ceramic Capacitor X5R 0402 10V 1 C3 0402ZD103MAT AVX(3) 1nF Ceramic Capacitor X5R 0402 10V 1 C3216X5R0J476K C4 GRM32ER60J476ME20 12106D476MAT2A C5 VJ0402A330KXAA D1 SSA33L RLF7030-1R0N6R4 L1 744 778 9001 IHLP2525AH-01 1 September 2007 TDK (1) 47F Ceramic Capacitor X5R 1206 6.3V Murata(2) (3) Vishay VT(4) (4) Vishay Semi TDK 1 47F Ceramic Capacitor X5R 1210 6.3V AVX (1) 33pF Ceramic Capacitor 0402 1 3A Schottky 30V SMA 1 1H Inductor 8.8m 7.1mm(L) x 6.8mm (W)x 3.2mm(H) Wurth Elektronik(5) (4) Vishay Dale 1H Inductor 12m 7.3mm(L)x7.3mm(W)x3.2mm(H) 1 1H Inductor 17.5m (L)6.47mmx(W)6.86mmx(H) 1.8mm 14 M9999-090707-C Micrel, Inc. R1 R2 R3 MIC2208 CRCW04024992F Vishay Dale(4) CRCW04023322F Vishay Dale(4) 33.3 k 1% 0402 For 2.5VOUT CRCW04026192F Vishay Dale(4) 61.9 k 1% 0402 For 1.8 VOUT CRCW04021003F (4) Vishay Dale 100 k 1% 0402 For 1.5 VOUT CRCW04022493F Vishay Dale(4) 249 k 1% 0402 For 1.2 VOUT Vishay Dale(4) Open For 1.0 VOUT CRCW04024991F 49.9K 1% 0402 Resistor (4) 499K 1% 0402 Resistor (4) Vishay Dale 1 1 R4 CRCW04024991F Vishay Dale 90.9K 1% 0402 Resistor 1 R5 CRCW040210R0F Vishay Dale(4) 10 1% 0402 Resistor 1 R6 CRCW04021002F Vishay Dale(4) 10K 1% 0402 Resistor 1 1MHz 3A Buck Regulator 1 U1 MIC2208BML (6) Micrel, Inc. Notes: 1. TDK: www.tdk.com 2. Murata: www.murata.com 3. AVX: www.avx.com 4. Vishay: www.vishay.com 5. Wurth Elektronik Midcom, Inc.: www.midcom-inc..com 6. Micrel, Inc.: www.micrel.com The network analyzer will then sweep the source while monitoring A and R for an A/R measurement. While this is the most common method for measuring the gain and phase of a power supply, it does have significant limitations. First, to measure low frequency gain and phase, the transformer needs to be high in inductance. This makes frequencies <100Hz require an extremely large and expensive transformer. Conversely, it must be able to inject high frequencies. Transformers with these wide frequency ranges generally need to be custom made and are extremely expensive (usually in the tune of several hundred dollars!). By using an op-amp, cost and frequency limitations used by an injection transformer are completely eliminated. Figure 8 demonstrates using an op-amp in a summing amplifier configuration for signal injection. Loop Stability and Bode Analysis Bode analysis is an excellent way to measure small signal stability and loop response in power supply designs. Bode analysis monitors gain and phase of a control loop. This is done by breaking the feedback loop and injecting a signal into the feedback node and comparing the injected signal to the output signal of the control loop. This will require a network analyzer to sweep the frequency and compare the injected signal to the output signal. The most common method of injection is the use of transformer. Figure 7 demonstrates how a transformer is used to inject a signal into the feedback network. Network Analyzer "R" Input +8V MIC922BC5 Feedback R3 1k Figure 7. Transformer Injection A 50 resistor allows impedance matching from the network analyzer source. This method allows the DC loop to maintain regulation and allow the network analyzer to insert an AC signal on top of the DC voltage. September 2007 R4 1k 50 R1 1k Network Analyzer "A" Input Output Network Analyzer Source Figure 8. Op Amp Injection 15 M9999-090707-C Micrel, Inc. MIC2208 R1 and R2 reduce the DC voltage from the output to the non-inverting input by half. The network analyzer is generally a 50 source. R1 and R2 also divide the AC signal sourced by the network analyzer by half. These two signals are "summed" together at half of their original input. The output is then gained up by 2 by R3 and R4 (the 50 is to balance the network analyzer's source impedance) and sent to the feedback signal. This essentially breaks the loop and injects the AC signal on top of the DC output voltage and sends it to the feedback. By monitoring the feedback "R" and output "A", gain and phase are measured. This method has no minimum frequency. Ensure that the bandwidth of the op-amp being used is much greater than the expected bandwidth of the power supplies control loop. An op-amp with >100MHz bandwidth is more than sufficient for most power supplies (which includes both linear and switching) and are more common and significantly cheaper than the injection transformers previously mentioned. The one disadvantage to using the op-amp injection method, that the supply voltages need to below the maximum operating voltage of the op-amp. Also, the maximum output voltage for driving 50 inputs using the MIC922 is 3V. For measuring higher output voltages, a 1M input impedance is required for the A and R channels. Remember to always measure the output voltage with an oscilloscope to ensure the measurement is working properly. You should see a single sweeping sinusoidal waveform without distortion on the output. If there is distortion of the sinusoid, reduce the amplitude of the source signal. You could be overdriving the feedback causing a large signal response. Figure 9. Output Impedance Measurement By setting up a network analyzer to sweep the feedback current, while monitoring the output of the voltage regulator and the voltage across the load resistance, output impedance is easily obtainable. To keep the current from being too high, a DC offset needs to be applied to the network analyzer's source signal. This can be done with an external supply and 50 resistor. Make sure that the currents are verified with an oscilloscope first, to ensure the integrity of the signal measurement. It is always a good idea to monitor the A and R measurements with a scope while you are sweeping it. To convert the network analyzer data from dBm to something more useful (such as peak-to-peak voltage and current in our case): 10 V = and peak to peak current: Output Impedance and Transient response 10 I = Output impedance, simply stated, is the amount of output voltage deviation vs. the load current deviation. The lower the output impedance, the better. Z OUT = dBm x 1mW x 50 x 2 10 0.707 x R LOAD The following graph shows output impedance vs. frequency at 2A load current sweeping the AC current from 10Hz to 10MHz, at 1A peak to peak amplitude. VOUT I OUT Output Impedance vs Frequency 1 Output Impedance (Ohms) Output impedance for a buck regulator is the parallel impedance of the output capacitor and the MOSFET and inductor divided by the gain: Z TOTAL dBm x 1mW x 50 x 2 10 0.707 R + DCR + X L = DSON || X COUT GAIN To measure output impedance vs. frequency, the load current must be load current must be swept across the frequencies measured, while the output voltage is monitored. Figure 9 shows a test set-up to measure output impedance from 10Hz to 1MHz using the MIC5190 high speed controller. 3.3V IN 0. 1 5V IN 0 . 01 V OUT = 1.8V L =1H COUT = 4.7F+0.1F 0. 0 0 1 10 10 0 1k 10 k 10 0 k 1M 10 M Frequency (Hz) September 2007 16 M9999-090707-C Micrel, Inc. MIC2208 From this graph, you can see the effects of bandwidth and output capacitance. For frequencies <100KHz, the output impedance is dominated by the gain and inductance. For frequencies >100KHz, the output impedance is dominated by the capacitance. A good approximation for transient response can be calculated from determining the frequency of the load step in amps per second: Ripple measurements To properly measure ripple on either input or output of a switching regulator, a proper ring in tip measurement is required. Standard oscilloscope probes come with a grounding clip, or a long wire with an alligator clip. Unfortunately, for high frequency measurements, this ground clip can pick-up high frequency noise and erroneously inject it into the measured output ripple. The standard evaluation board accommodates a home made version by providing probe points for both the input and output supplies and their respective grounds. This requires the removing of the oscilloscope probe sheath and ground clip from a standard oscilloscope probe and wrapping a non-shielded bus wire around the oscilloscope probe. If there does not happen to be any non shielded bus wire immediately available, the leads from axial resistors will work. By maintaining the shortest possible ground lengths on the oscilloscope probe, true ripple measurements can be obtained A/sec 2 Then, determine the output impedance by looking at the output impedance vs. frequency graph. Then calculating the voltage deviation times the load step: VOUT = IOUT x ZOUT The output impedance graph shows the relationship between supply voltage and output impedance. This is caused by the lower RDSON of the high side MOSFET and the increase in gain with increased supply voltages. This explains why higher supply voltages have better transient response. f = Z TOTAL = September 2007 R DSON + DCR + X L GAIN || X COUT 17 M9999-090707-C Micrel, Inc. MIC2208 Package Information 12-Pin MLF(R) (ML) MICREL, INC. 2180 FORTUNE DRIVE SAN JOSE, CA 95131 USA TEL +1 (408) 944-0800 FAX +1 (408) 474-1000 WEB http://www.micrel.com The information furnished by Micrel in this data sheet is believed to be accurate and reliable. However, no responsibility is assumed by Micrel for its use. Micrel reserves the right to change circuitry and specifications at any time without notification to the customer. Micrel Products are not designed or authorized for use as components in life support appliances, devices or systems where malfunction of a product can reasonably be expected to result in personal injury. Life support devices or systems are devices or systems that (a) are intended for surgical implant into the body or (b) support or sustain life, and whose failure to perform can be reasonably expected to result in a significant injury to the user. A Purchaser's use or sale of Micrel Products for use in life support appliances, devices or systems is a Purchaser's own risk and Purchaser agrees to fully indemnify Micrel for any damages resulting from such use or sale. (c) 2005 Micrel, Incorporated. September 2007 18 M9999-090707-C