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 MIC2168
Micrel
MIC2168
1MHz PWM Synchronous Buck Control IC
General Description
The MIC2168 is a high-efficiency, simple to use 1MHz PWM synchronous buck control IC housed in a small MSOP-10 package. The MIC2168 allows compact DC/DC solutions with a minimal external component count and cost. The MIC2168 operates from a 3V to 14.5V input, without the need of any additional bias voltage. The output voltage can be precisely regulated down to 0.8V. The adaptive all N-Channel MOSFET drive scheme allows efficiencies over 95% across a wide load range. The MIC2168 senses current across the high-side N-Channel MOSFET, eliminating the need for an expensive and lossy current-sense resistor. Current limit accuracy is maintained by a positive temperature coefficient that tracks the increasing RDS(ON) of the external MOSFET. Further cost and space are saved by the internal in-rush-current limiting digital soft-start. The MIC2168 is available in a 10-pin MSOP package, with a wide junction operating range of -40C to +125C. All support documentation can be found on Micrel's web site at www.micrel.com.
Features
* * * * * * * * * * * * * * * * * * * * * 3V to 14.5V input voltage range Adjustable output voltage down to 0.8V Up to 95% efficiency 1MHz PWM operation Adjustable current-limit senses high-side N-Channel MOSFET current No external current sense resistor Adaptive gate drive increases efficiency Ultra-fast response with hysteretic transient recovery mode Overvoltage protection protects the load in fault conditions Dual mode current limit speeds up recovery time Hiccup mode short-circuit protection Internal soft-start Dual function COMP and EN pin allows low-power shutdown Small size MSOP 10-lead package Point-of-load DC/DC conversion Set-top boxes Graphic cards LCD power supplies Telecom power supplies Networking power supplies Cable modems and routers
Applications
Typical Application
VIN = 5V SD103BWS 100F 4.7F
100 95 90
EFFICIENCY (%)
0.1F
MIC2168 Efficiency
VDD
BST CS HSD VSW
1k IRF7821 1.2H 3.3V 10k 150F x 2 3.24k
85 80 75 70 65 60 55 50 VIN = 5V VOUT = 3.3V 0 2 4 6 ILOAD (A) 8 10
VIN
MIC2168
COMP/EN 100pF 4k 100nF GND LSD FB
IRF7821
MIC2168 Adjustable Output 1MHz Converter
Micrel, Inc. * 1849 Fortune Drive * San Jose, CA 95131 * USA * tel + 1 (408) 944-0800 * fax + 1 (408) 944-0970 * http://www.micrel.com
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Ordering Information
Part Number MIC2168BMM Frequency 1MHz Junction Temp. Range -40C to +125C Package 10-lead MSOP
Pin Configuration
VIN VDD CS COMP/EN FB 1 2 3 4 5 10 9 8 7 6 BST HSD VSW LSD GND
10-Pin MSOP (MM)
Pin Description
Pin Number 1 2 Pin Name VIN VDD Pin Function Supply Voltage (Input): 3V to 14.5V. 5V Internal Linear Regulator (Output): VDD is the external MOSFET gate drive supply voltage and an internal supply bus for the IC. When VIN is <5V, this regulator operates in dropout mode. Current Sense / Enable (Input): Current-limit comparator noninverting input. The current limit is sensed across the MOSFET during the ON time. The current can be set by the resistor in series with the CS pin. Compensation (Input): Dual function pin. Pin for external compensation. If this pin is pulled below 0.2V, with the reference fully up the device shuts down (50A typical current draw). Feedback (Input): Input to error amplifier. Regulates error amplifier to 0.8V. Ground (Return). Low-Side Drive (Output): High-current driver output for external synchronous MOSFET. Switch (Return): High-side MOSFET driver return. High-Side Drive (Output): High-current output-driver for the high-side MOSFET. When VIN is between 3.0V to 5V, 2.5V threshold-rated MOSFETs should be used. At VIN > 5V, 5V threshold MOSFETs should be used. Boost (Input): Provides the drive voltage for the high-side MOSFET driver. The gate-drive voltage is higher than the source voltage by VIN minus a diode drop.
3
CS
4
COMP/EN
5 6 7 8 9
FB GND LSD VSW HSD
10
BST
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Absolute Maximum Ratings(1)
Supply Voltage (VIN) .................................................. 15.5V Booststrapped Voltage (VBST) ............................... VIN +5V Junction Temperature (TJ) ................. -40C TJ +125C Storage Temperature (TS) ....................... -65C to +150C
Operating Ratings(2)
Supply Voltage (VIN) .................................... +3V to +14.5V Output Voltage Range ........................... 0.8V to VIN x DMAX Package Thermal Resistance JA 10-lead MSOP ............................................ 180C/W
Electrical Characteristics(3)
TJ = 25C, VIN = 5V, unless otherwise specified. Bold values indicate -40C < TJ < +125C Parameter Feedback Voltage Reference Feedback Voltage Reference Feedback Bias Current Output Voltage Line Regulation Output Voltage Load Regulation Output Voltage Total Regulation Oscillator Section Oscillator Frequency Maximum Duty Cycle Minimum On-Time(4) 900 90 30 60 1000 1100 kHz % ns 3V VIN 14.5V; 1A IOUT 10A; (VOUT = 2.5V)(4) Condition ( 1%) ( 2% over temp) Min 0.792 0.784 Typ 0.8 0.8 30 0.03 0.5 0.6 Max 0.808 0.816 100 Units V V nA %/V % %
Input and VDD Supply PWM Mode Supply Current Shutdown Quiescent Current VCOMP Shutdown Threshold VCOMP Shutdown Blanking Period Digital Supply Voltage (VDD)
Notes: 1. Absolute maximum ratings indicate limits beyond which damage to the component may occur. Electrical specifications do not apply when operating the device outside of its operating ratings. The maximum allowable power dissipation is a function of the maximum junction temperature, TJ(max), the junction-to-ambient thermal resistance, JA, and the ambient temperature, TA. The maximum allowable power dissipation will result in excessive die temperature, and the regulator will go into thermal shutdown. 2. Devices are ESD sensitive, handling precautions required. 3. Specification for packaged product only. 4. Guaranteed by design.
VCS = VIN -0.25V; VFB = 0.7V (output switching but excluding external MOSFET gate current.) VCOMP/EN = 0V 0.1 CCOMP = 100nF VIN 6V 4.7
1.6 50 0.25 4 5
3 150 0.4
mA A V ms
5.3
V
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Electrical Characteristics(5)
Parameter Error Amplifier DC Gain Transconductance Soft-Start Soft-Start Current Current Sense CS Over Current Trip Point Temperature Coefficient Output Fault Correction Thresholds Upper Threshold, VFB_OVT Lower Threshold, VFB_UVT Gate Drivers Rise/Fall Time Output Driver Impedance Into 3000pF at VIN > 5V Source, VIN = 5V Sink, VIN = 5V Source, VIN = 3V Sink, VIN = 3V Driver Non-Overlap Time
Notes: 5. Specification for packaged product only. 6. Guaranteed by design.
Condition
Min
Typ
Max
Units
70 1
dB ms A A ppm/C
After timeout of internal timer. See "Soft-Start" section.
8.5
VCS = VIN -0.25V
160
200 +1800
240
(relative to VFB) (relative to VFB)
+3 -3
% %
30 6 6 10 10 10 20
ns ns
Note 6
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Typical Characteristics
VIN = 5V
PWM Mode Supply Current vs. Temperature
PWM Mode Supply Current vs. Supply Voltage
2.9 2.7 2.5 2.3 2.1 1.9 1.7 1.5 1.3 1.1 0.9 0.7 0.5 -40 -20 0 20 40 60 80 100120140 TEMPERATURE (C)
2.0 QUIESCENT CURRENT (mA)
0.820 0.815 0.810
VFB Line Regulation
1.5
IDD (mA)
VFB (V)
1.0 0.5
0.805 0.800 0.795 0.790 0.785
0
5 10 SUPPLY VOLTAGE (V)
15
0.780
0
5 VIN (V)
10
15
VFB vs. Temperature
0.820 0.815 0.810
VFB (V)
VDD Line Regulation
VDD REGULATOR VOLTAGE (V)
6 5 4
5.01 4.99 4.97 4.95 4.93 4.91 4.89 4.87 4.85 0
VDD Load Regulation
0.800 0.795 0.790 0.785 0.780 -60 -30 0 30 60 90 120 150 TEMPERATURE (C)
VDD (V)
0.805
3 2 1 0 0 5 VIN (V) 10 15
5 10 15 20 25 LOAD CURRENT (mA)
30
5.0
VDD LINE REGULATION (%)
VDD Line Regulation vs. Temperature
1200 1150
FREQUENCY (kHz)
Oscillator Frequency vs. Temperature
1.5
FREQUENCY VARIATION (%)
Oscillator Frequency vs. Supply Voltage
4.5 4.0 3.5 3.0 2.5 2.0 1.5 1.0 0.5 0.0 -60 -30 0 30 60 90 120 150 TEMPERATURE (C)
1.0 0.5 0 -0.5 -1.0 -1.5 0 5 10 SUPPLY VOLTAGE (V) 15
1100 1050 1000 950 900 850 800 -60 -30 0 30 60 90 120 150 TEMPERATURE (C)
4
Current Limit Foldback
240 220
Overcurrent Trip Point vs. Temperature
3
VOUT (V) ICS (A)
200 180 160 140 120
2
1
Top MOSFET = Si4800 RCS = 1k
0
0
2
4 6 ILOAD (A)
8
10
100 -60 -30 0 30 60 90 120 150 TEMPERATURE (C)
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Functional Diagram
CIN VIN RCS CS VDD
5V LDO
5V
VDD 5V
Current Limit Comparator
High-Side Driver
D1 HSD Q1 BOOST 4 RSW CBST L1 VOUT
Bandgap Reference
0.8V BG Valid
Current Limit Reference
SW
5V Clamp & Startup Current
Driver Logic
5V
COUT
Soft-Start & Digital Delay Counter
Ramp Clock
Enable Error Loop 0.8V
Low-Side Driver
LSD
Q2
PWM
Comparator
VREF +3%
FB Hys
Comparator
Error Amp
VREF 3%
R3
R2
MIC2168
COMP GND
C1 C2 R1
MIC2168 Block Diagram
Functional Description
The MIC2168 is a voltage mode, synchronous step-down switching regulator controller designed for high output power without the use of an external sense resistor. It includes an internal soft-start function which reduces the power supply input surge current at start-up by controlling the output voltage rise time, a PWM generator, a reference voltage, two MOSFET drivers, and short-circuit current limiting circuitry to form a complete 1MHz switching regulator. Theory of Operation The MIC2168 is a voltage mode step-down regulator. The figure above illustrates the block diagram for the voltage control loop. The output voltage variation due to load or line changes will be sensed by the inverting input of the transconductance error amplifier via the feedback resistors R3, and R2 and compared to a reference voltage at the noninverting input. This will cause a small change in the DC voltage level at the output of the error amplifier which is the input to the PWM comparator. The other input to the comparator is a 0 to 1V triangular waveform. The comparator generates a rectangular waveform whose width tON is equal to the time from the start of the clock cycle t0 until t1, the time the triangle crosses the output waveform of the error amplifier. To illustrate the control loop, let us assume the output voltage drops due to sudden load turn-on, this would cause 6
the inverting input of the error amplifier which is divided down version of VOUT to be slightly less than the reference voltage causing the output voltage of the error amplifier to go high. This will cause the PWM comparator to increase tON time of the top side MOSFET, causing the output voltage to go up and bringing VOUT back in regulation. Soft-Start The COMP/EN pin on the MIC2168 is used for the following three functions: 1. Disables the part by grounding this pin 2. External compensation to stabilize the voltage control loop 3. Soft-start For better understanding of the soft-start feature, let's assume VIN = 12V, and the MIC2168 is allowed to power-up by un-grounding the COMP/EN pin. The COMP pin has an internal 8.5A current source that charges the external compensation capacitor. As soon as this voltage rises to 180mV (t = Cap_COMP x 0.18V/8.5A), the MIC2168 allows the internal VDD linear regulator to power up and as soon as it crosses the undervoltage lockout of 2.6V, the chip's internal oscillator starts switching. At this point in time, the COMP pin current source increases to 40A and an internal 11-bit counter starts counting which takes approximately 2ms to complete. During counting, the COMP voltage is clamped at November 2003
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0.65V. After this counting cycle the COMP current source is reduced to 8.5A and the COMP pin voltage rises from 0.65V to 0.95V, the bottom edge of the saw-tooth oscillator. This is the beginning of 0% duty cycle and it increases slowly causing the output voltage to rise slowly. The MIC2168 has two hysteretic comparators that are enabled when VOUT is within 3% of steady state. When the output voltage reaches 97% of programmed output voltage, then the gm error amplifier is enabled along with the hysteretic comparator. This point onwards, the voltage control loop (gm error amplifier) is fully in control and will regulate the output voltage. Soft-start time can be calculated approximately by adding the following four time frames: t1 = Cap_COMP x 0.18V/8.5A t2 = 12 bit counter, approx 2ms t3 = Cap_COMP x 0.3V/8.5A
V Cap_COMP t4 = OUT x 0.5 x 8.5A VIN
Micrel
The current limiting resistor RCS is calculated by the following equation:
RCS =
RDS(ON) Q1 x IL 200A
Equation (1)
IL = ILOAD + where:
1 2(Inductor Ripple Current)
Inductor Ripple Current = VOUT x
VIN x FSWITCHING x L
(VIN - VOUT )
Soft-Start Time(Cap_COMP=100nF) = t1 + t2 + t3 + t4 = 2.1ms + 2ms + 3.5ms + 1.8ms = 10ms Current Limit The MIC2168 uses the RDS(ON) of the top power MOSFET to measure output current. Since it uses the drain to source resistance of the power MOSFET, it is not very accurate. This scheme is adequate to protect the power supply and external components during a fault condition by cutting back the time the top MOSFET is on if the feedback voltage is greater than 0.67V. In case of a hard short when feedback voltage is less than 0.67V, the MIC2168 discharges the COMP capacitor to 0.65V, resets the digital counter and automatically shuts off the top gate drive, and the gm error amplifier and the -3% hysteretic comparators are completely disabled and the softstart cycles restarts. This mode of operation is called the "hiccup mode" and its purpose is to protect the down stream load in case of a hard short. The circuit in Figure 1 illustrates the MIC2168 current limiting circuit.
VIN C2 CIN 0 RCS CS LSD L1 Inductor Q2 MOSFET N C1 COUT HSD Q1 MOSFET N VOUT
200A
Figure 1. The MIC2168 Current Limiting Circuit
FSWITCHING = 1MHz 200A is the internal sink current to program the MIC2168 current limit. The MOSFET RDS(ON) varies 30% to 40% with temperature; therefore, it is recommended to add a 50% margin to the load current (ILOAD) in the above equation to avoid false current limiting due to increased MOSFET junction temperature rise. It is also recommended to connect RCS resistor directly to the drain of the top MOSFET Q1, and the RSW resistor to the source of Q1 to accurately sense the MOSFETs RDS(ON). A 0.1F capacitor in parallel with RCS should be connected to filter some of the switching noise. Internal VDD Supply The MIC2168 controller internally generates VDD for self biasing and to provide power to the gate drives. This VDD supply is generated through a low-dropout regulator and generates 5V from VIN supply greater than 5V. For supply voltage less than 5V, the VDD linear regulator is approximately 200mV in dropout. Therefore, it is recommended to short the VDD supply to the input supply through a 10 resistor for input supplies between 2.9V to 5V. MOSFET Gate Drive The MIC2168 high-side drive circuit is designed to switch an N-Channel MOSFET. The block diagram in Figure 2 shows a bootstrap circuit, consisting of D2 and CBST, supplies energy to the high-side drive circuit. Capacitor CBST is charged while the low-side MOSFET is on and the voltage on the VSW pin is approximately 0V. When the high-side MOSFET driver is turned on, energy from CBST is used to turn the MOSFET on. As the MOSFET turns on, the voltage on the VSW pin increases to approximately VIN. Diode D2 is reversed biased and CBST floats high while continuing to keep the high-side MOSFET on. When the low-side switch is turned back on, CBST is recharged through D2. The drive voltage is derived from the internal 5V VDD bias supply. The nominal low-side gate drive voltage is 5V and the nominal high-side gate drive voltage is approximately 4.5V due the voltage drop across D2. An approximate 20ns delay between the high- and low-side driver transitions is used to prevent current from simultaneously flowing unimpeded through both MOSFETs. MOSFET Selection The MIC2168 controller works from input voltages of 3V to 13.2V and has an internal 5V regulator to provide power to turn the external N-Channel power MOSFETs for high- and 7
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low-side switches. For applications where VIN < 5V, the internal VDD regulator operates in dropout mode, and it is necessary that the power MOSFETs used are low threshold and are in full conduction mode for VGS of 2.5V. For applications when VIN > 5V; logic-level MOSFETs, whose operation is specified at VGS = 4.5V must be used. It is important to note the on-resistance of a MOSFET increases with increasing temperature. A 75C rise in junction temperature will increase the channel resistance of the MOSFET by 50% to 75% of the resistance specified at 25C. This change in resistance must be accounted for when calculating MOSFET power dissipation and in calculating the value of current-sense (CS) resistor. Total gate charge is the charge required to turn the MOSFET on and off under specified operating conditions (VDS and VGS). The gate charge is supplied by the MIC2168 gate drive circuit. At 1MHz switching frequency and above, the gate charge can be a significant source of power dissipation in the MIC2168. At low output load, this power dissipation is noticeable as a reduction in efficiency. The average current required to drive the high-side MOSFET is:
IG[high-side](avg) = QG x fS
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The power dissipated in the switching transistor is the sum of the conduction losses during the on-time (PCONDUCTION) and the switching losses that occur during the period of time when the MOSFETs turn on and off (PAC).
PSW = PCONDUCTION + PAC
where:
PCONDUCTION = ISW(rms)2 x RSW
PAC = PAC(off) + PAC(on) RSW = on-resistance of the MOSFET switch
V D = duty cycle O VIN
Making the assumption the turn-on and turn-off transition times are equal; the transition times can be approximated by: tT = CISS x VGS + COSS x VIN IG
where: IG[high-side](avg) = average high-side MOSFET gate current. QG = total gate charge for the high-side MOSFET taken from manufacturer's data sheet for VGS = 5V. The low-side MOSFET is turned on and off at VDS = 0 because the freewheeling diode is conducting during this time. The switching loss for the low-side MOSFET is usually negligible. Also, the gate-drive current for the low-side MOSFET is more accurately calculated using CISS at VDS = 0 instead of gate charge. For the low-side MOSFET:
IG[low-side](avg) = CISS x VGS x fS
where: CISS and COSS are measured at VDS = 0 IG = gate-drive current (1A for the MIC2168) The total high-side MOSFET switching loss is:
PAC = (VIN +VD ) x IPK x t T x fS
where: tT = switching transition time (typically 20ns to 50ns) VD = freewheeling diode drop, typically 0.5V fS it the switching frequency, nominally 1MHz The low-side MOSFET switching losses are negligible and can be ignored for these calculations. Inductor Selection Values for inductance, peak, and RMS currents are required to select the output inductor. The input and output voltages and the inductance value determine the peak-to-peak inductor ripple current. Generally, higher inductance values are used with higher input voltages. Larger peak-to-peak ripple currents will increase the power dissipation in the inductor and MOSFETs. Larger output ripple currents will also require more output capacitance to smooth out the larger ripple current. Smaller peak-to-peak ripple currents require a larger inductance value and therefore a larger and more expensive inductor. A good compromise between size, loss and cost is to set the inductor ripple current to be equal to 20% of the maximum output current. The inductance value is calculated by the equation below.
Since the current from the gate drive comes from the input voltage, the power dissipated in the MIC2168 due to gate drive is: PGATEDRIVE = VIN IG[high-side](avg) + IG[low-side](avg)
(
)
A convenient figure of merit for switching MOSFETs is the on resistance times the total gate charge RDS(ON) x QG. Lower numbers translate into higher efficiency. Low gate-charge logic-level MOSFETs are a good choice for use with the MIC2168. Parameters that are important to MOSFET switch selection are: * Voltage rating * On-resistance * Total gate charge The voltage ratings for the top and bottom MOSFET are essentially equal to the input voltage. A safety factor of 20% should be added to the VDS(max) of the MOSFETs to account for voltage spikes due to circuit parasitics.
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L=
VOUT x (VIN (max) - VOUT ) VIN (max) x fS x 0.2 x IOUT (max)
where: fS = switching frequency, 1MHz 0.2 = ratio of AC ripple current to DC output current VIN(max) = maximum input voltage 8 November 2003
MIC2168
The peak-to-peak inductor current (AC ripple current) is:
Micrel
feedback loop from stability point of view. See "Feedback Loop Compensation" section for more information. The maximum value of ESR is calculated: RESR VOUT IPP
IPP =
VOUT x (VIN (max) - VOUT ) VIN (max) x fS x L
The peak inductor current is equal to the average output current plus one half of the peak-to-peak inductor ripple current.
IPK = IOUT (max) + 0.5 x IPP
The RMS inductor current is used to calculate the I2 x R losses in the inductor.
where: VOUT = peak-to-peak output voltage ripple IPP = peak-to-peak inductor ripple current The total output ripple is a combination of the ESR output capacitance. The total ripple is calculated below:
I x (1- D) 2 PP + IPP x RESR COUT x fS
2
IINDUCTOR(rms)
1 IP = IOUT (max) x 1 + 3 IOUT (max)
2
VOUT =
(
)
Maximizing efficiency requires the proper selection of core material and minimizing the winding resistance. The high frequency operation of the MIC2168 requires the use of ferrite materials for all but the most cost sensitive applications. Lower cost iron powder cores may be used but the increase in core loss will reduce the efficiency of the power supply. This is especially noticeable at low output power. The winding resistance decreases efficiency at the higher output current levels. The winding resistance must be minimized although this usually comes at the expense of a larger inductor. The power dissipated in the inductor is equal to the sum of the core and copper losses. At higher output loads, the core losses are usually insignificant and can be ignored. At lower output currents, the core losses can be a significant contributor. Core loss information is usually available from the magnetics vendor. Copper loss in the inductor is calculated by the equation below:
where: D = duty cycle COUT = output capacitance value fS = switching frequency The voltage rating of capacitor should be twice the voltage for a tantalum and 20% greater for an aluminum electrolytic. The output capacitor RMS current is calculated below: IC = IPP 12
= IC x RESR(C
OUT(rms)
The power dissipated in the output capacitor is:
PDISS(C
OUT ) OUT(rms)2 OUT )
PINDUCTORCu = IINDUCTOR(rms)2 x R WINDING
The resistance of the copper wire, RWINDING, increases with temperature. The value of the winding resistance used should be at the operating temperature.
R WINDING(hot) = R WINDING(20C) x 1 + 0.0042 x (THOT - T20C )
(
)
where: THOT = temperature of the wire under operating load T20C = ambient temperature RWINDING(20C) is room temperature winding resistance (usually specified by the manufacturer) Output Capacitor Selection The output capacitor values are usually determined capacitors ESR (equivalent series resistance). Voltage and RMS current capability are two other important factors selecting the output capacitor. Recommended capacitors tantalum, low-ESR aluminum electrolytics, and POSCAPS. The output capacitor's ESR is usually the main cause of output ripple. The output capacitor ESR also affects the overall voltage
Input Capacitor Selection The input capacitor should be selected for ripple current rating and voltage rating. Tantalum input capacitors may fail when subjected to high inrush currents, caused by turning the input supply on. Tantalum input capacitor voltage rating should be at least 2 times the maximum input voltage to maximize reliability. Aluminum electrolytic, OS-CON, and multilayer polymer film capacitors can handle the higher inrush currents without voltage derating. The input voltage ripple will primarily depend on the input capacitor's ESR. The peak input current is equal to the peak inductor current, so:
VIN = IINDUCTOR(peak) x RESR(C ) IN
The input capacitor must be rated for the input current ripple. The RMS value of input capacitor current is determined at the maximum output current. Assuming the peak-to-peak inductor ripple current is low:
ICIN (rms) IOUT (max) x D x (1- D)
The power dissipated in the input capacitor is: PDISS(C
IN )
= IC
IN (rms)
2
x RESR(C
IN )
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Voltage Setting Components The MIC2168 requires two resistors to set the output voltage as shown in Figure 2.
R1 Error Amp FB
7
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decrease high frequency noise. If the MOSFET body diode is used, it must be rated to handle the peak and average current. The body diode has a relatively slow reverse recovery time and a relatively high forward voltage drop. The power lost in the diode is proportional to the forward voltage drop of the diode. As the high-side MOSFET starts to turn on, the body diode becomes a short circuit for the reverse recovery period, dissipating additional power. The diode recovery and the circuit inductance will cause ringing during the high-side MOSFET turn-on. An external Schottky diode conducts at a lower forward voltage preventing the body diode in the MOSFET from turning on. The lower forward voltage drop dissipates less power than the body diode. The lack of a reverse recovery mechanism in a Schottky diode causes less ringing and less power loss. Depending on the circuit components and operating conditions, an external Schottky diode will give a 1/2% to 1% improvement in efficiency. Feedback Loop Compensation The MIC2168 controller comes with an internal transconductance error amplifier used for compensating the voltage feedback loop by placing a capacitor (C1) in series with a resistor (R1) and another capacitor C2 in parallel from the COMP pin to ground. See "Functional Block Diagram." Power Stage The power stage of a voltage mode controller has an inductor, L1, with its winding resistance (DCR) connected to the output capacitor, COUT, with its electrical series resistance (ESR) as shown in Figure 3. The transfer function G(s), for such a system is:
L DCR VO ESR COUT
R2
VREF 0.8V MIC2168 [adj.]
Figure 2. Voltage-Divider Configuration Where: VREF for the MIC2168 is typically 0.8V The output voltage is determined by the equation: R1 VO = VREF x 1 + R2 A typical value of R1 can be between 3k and 10k. If R1 is too large, it may allow noise to be introduced into the voltage feedback loop. If R1 is too small, in value, it will decrease the efficiency of the power supply, especially at light loads. Once R1 is selected, R2 can be calculated using: R2 = VREF x R1 VO - VREF
External Schottky Diode An external freewheeling diode is used to keep the inductor current flow continuous while both MOSFETs are turned off. This dead time prevents current from flowing unimpeded through both MOSFETs and is typically 15ns. The diode conducts twice during each switching cycle. Although the average current through this diode is small, the diode must be able to handle the peak current.
ID(avg) = IOUT x 2 x 80ns x fS
The reverse voltage requirement of the diode is:
VDIODE(rrm) = VIN
Figure 3. The Output LC Filter in a Voltage Mode Buck Converter
(1+ ESR x s x C) G(s) = 2 x L x C + 1 + ESR x s x C DCR x s x C + s
The power dissipated by the Schottky diode is:
PDIODE = ID(avg) x VF
where: VF = forward voltage at the peak diode current The external Schottky diode, D1, is not necessary for circuit operation since the low-side MOSFET contains a parasitic body diode. The external diode will improve efficiency and
Plotting this transfer function with the following assumed values (L=2 H, DCR=0.009, COUT=1000F, ESR=0.050) gives lot of insight as to why one needs to compensate the loop by adding resistor and capacitors on the COMP pin. Figures 4 and 5 show the gain curve and phase curve for the above transfer function.
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30 30
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00 50
PHASE
7.5
GAIN
15
100
37.5
150
60 60 100 100 1.10
3
180
1 .10 f
4
1 .10
5
1 .10
6
1000000
100 100
1.103
1 .104 f
1 .105
1 .106 1000000
Figure 4. The Gain Curve for G(s)
Figure 6. The Phase Curve with ESR = 0.002 It can be seen from Figure 5 that at 50kHz, the phase is approximately -90 versus Figure 6 where the number is -150. This means that the transconductance error amplifier has to provide a phase boost of about 45 to achieve a closed loop phase margin of 45 at a crossover frequency of 50kHz for Figure 4, versus 105 for Figure 6. The simple RC and C2 compensation scheme allows a maximum error amplifier phase boost of about 90. Therefore, it is easier to stabilize the MIC2168 voltage control loop by using high ESR value output capacitors. gm Error Amplifier
00 50 PHASE 100 150 180 100 100 1.103 1 .104 f 1 .105 1 .106 1000000
Figure 5. Phase Curve for G(s) It can be seen from the transfer function G(s) and the gain curve that the output inductor and capacitor create a two pole system with a break frequency at: fLC = 1 2 x L x COUT
It is undesirable to have high error amplifier gain at high frequencies because high frequency noise spikes would be picked up and transmitted at large amplitude to the output, thus, gain should be permitted to fall off at high frequencies. At low frequency, it is desired to have high open-loop gain to attenuate the power line ripple. Thus, the error amplifier gain should be allowed to increase rapidly at low frequencies. The transfer function with R1, C1, and C2 for the internal gm error amplifier can be approximated by the following equation:
1 + R1x S x C1 Error Amplifier(z) = gm x s x C1 + C2 1 + R1x C1x C2 x S ( ) C1 + C2
Therefore, fLC = 3.6kHz By looking at the phase curve, it can be seen that the output capacitor ESR (0.050) cancels one of the two poles (LCOUT) system by introducing a zero at:
fZERO = 1 2 x x ESR x COUT
The above equation can be simplified by assuming C2<Therefore, FZERO = 6.36kHz. From the point of view of compensating the voltage loop, it is recommended to use higher ESR output capacitors since they provide a 90 phase gain in the power path. For comparison purposes, Figure 6, shows the same phase curve with an ESR value of 0.002.
1 + R1x S x C1 Error Amplifier(z) = gm x s x (C1)(1 + R1x C2 x S)
From the above transfer function, one can see that R1 and C1 introduce a zero and R1 and C2 a pole at the following frequencies: Fzero= 1/2 x R1 x C1 Fpole = 1/2 x C2 x R1 Fpole@origin = 1/2 x C1
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M9999-111803
MIC2168
Figures 7 and 8 show the gain and phase curves for the above transfer function with R1 = 9.3k, C1 = 1000pF, C2 = 100pF, and gm = .005-1. It can be seen that at 50kHz, the error amplifier exhibits approximately 45 of phase margin.
60 60
Micrel
100 71.607
OPEN LOOP GAIN MARGIN
50
ERROR AMPLIFIER GAIN
40
0
20
42.933 50 100 100
3 1.10
1 .10 f
4
1 .10
5
1 .10 1000000
6
Figure 9. Open-Loop Gain Margin
.001 1 .10
3
1 .10
4
1 .10 f
5
1 .10
6
1 .10
7
250 269.097
1000
10000000
Figure 7. Error Amplifier Gain Curve
200 215.856
OPEN LOOP PHASE MARGIN
300
ERROR AMPLIFIER PHASE
220
350 360
240
10 10
100
3 1.10
1 .10 f
4
1 .10
5
6 1 .10 1000000
Figure 10. Open-Loop Phase Margin
260 270 10 10 100 . 1 10
3
1 .10 f
4
1 .10
5
1 .10
6
1000000
Figure 8. Error Amplifier Phase Curve Total Open-Loop Response The open-loop response for the MIC2168 controller is easily obtained by adding the power path and the error amplifier gains together, since they already are in Log scale. It is desirable to have the gain curve intersect zero dB at tens of kilohertz, this is commonly called crossover frequency; the phase margin at crossover frequency should be at least 45. Phase margins of 30 or less cause the power supply to have substantial ringing when subjected to transients, and have little tolerance for component or environmental variations. Figures 9 and 10 show the open-loop gain and phase margin. It can be seen from Figure 9 that the gain curve intersects the 0dB at approximately 50kHz, and from Figure 10 that at 50kHz, the phase shows approximately 50 of margin.
M9999-111803
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MIC2168
Design Example Layout and Checklist: 1. Connect the current limiting (CS) resistor directly to the drain of top MOSFET Q1. 2. Connect the VSW pin directly to the source of top MOSFET Q1 thru a 4 to 10 resistor. The purpose of this resistor is to filter the switch node. 3. The feedback resistors R1 and R2 should be placed close to the FB pin. The top side of R1 should connect directly to the output node. Run this trace away from the switch node (junction of Q1, Q2, and L1). The bottom side of R1 should connect to the GND pin on the MIC2168. 4. The compensation resistor and capacitors should be placed right next to the COMP/EN pin and the other side should connect directly to the GND pin on the MIC2168 rather than going to the plane. 5. The input bulk capacitors should be placed close to the drain of the top MOSFET. 6. The 1F ceramic capacitor should be placed right on the VIN pin of the MIC2168. 7. The 4.7F to 10F ceramic capacitor should be placed right on the VDD pin. 8. The source of the bottom MOSFET should connect directly to the input capacitor GND with a thick trace. The output capacitor and the input capacitor should connect directly to the GND plane. 9. Place a 0.1F ceramic capacitor in parallel with the CS resistor to filter any switching noise.
Micrel
November 2003
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M9999-111803
MIC2168
Micrel
Package Information
Rev. 00
10-Pin MSOP (MM)
MICREL, INC. 1849 FORTUNE DRIVE
TEL
SAN JOSE, CA 95131
WEB
USA
+ 1 (408) 944-0800
FAX
+ 1 (408) 944-0970
http://www.micrel.com
The information furnished by Micrel in this datasheet 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 at Purchaser's own risk and Purchaser agrees to fully indemnify Micrel for any damages resulting from such use or sale. (c) 2003 Micrel, Incorporated. M9999-111803
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November 2003


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