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MIC2155 Datasheet(PDF) 29 Page - Micrel Semiconductor |
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MIC2155 Datasheet(HTML) 29 Page - Micrel Semiconductor |
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29 / 33 page ![]() Micrel, Inc. MIC2155/2156 May 2009 29 M9999-052709-A (408) 944-0800 Step 3: Determine the gain boost needed at the crossover frequency (fc) Typically, 50° of phase margin can be used for most applications. This is a good tradeoff between an overdamped system (slower response to transients) and an underdamped system (overshoot or unstable response to transients). It also allows some margin for component tolerances and variations due to ambient temperature changes. The phase margin at the crossover frequency (fc) can be determined by plotting the Gvd(s) phase on a bode plot or can be estimated with the following formula: ⎥⎦ ⎤ ⎢⎣ ⎡ + ⎥ ⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ − × = ϕ − − fz fc tan fo fc 1 fo Q fc tan 1 2 1 M The additional phase boost required from the error amplifier is: M Boost 52 ϕ − ° = ϕ Step 4: Determine the frequencies fz2 and fp1 The frequencies for the zero and pole (fz2 and fp1) are calculated for the desired amount of phase boost at the crossover frequency (fc). [] [] [] [] Boost Boost Boost Boost sin 1 sin 1 fc 1 fp sin 1 sin 1 fc 2 fz ϕ − ϕ + × = ϕ + ϕ − × = Step 5: Determine the frequency for fz1 The low frequency zero, fz1, is initially set to one-fifth of the LC resonant frequency. If it is set too low, it will force the low frequency gain to be low and impact transient response. If set too high, it will not add enough phase boost at the LC resonant frequency. This could cause conditional stability, which when the phase drops below - 180° before the gain crosses 0dB. If the DC gain should drop in this situation, this may lead to an unstable system. 5 fo 2 fz = Step 6: Determine the frequency for fp2 This is the high frequency pole, which is useful in additional attenuation of the switching frequency. It should initially be set at half of the switching frequency. If it is set too low, it will lower the phase margin at the crossover frequency, making it difficult to achieve the proper phase margin. If set too high, it will not provide attenuation of the switching frequency, which could lead to jitter of the switching waveform or instability under certain conditions. 2 fs 2 fp = Calculating Error Amplifier Component Values Once the pole and zero frequencies have been fixed, the error amplifier’s resistor and capacitor values are calculated. R1 This value is chosen first. All other component values are calculated from R1. A value of 10K is suggested. If R1 is chosen too high, R2 may be very large and the high impedances could be sensitive to noise. If the remote sense amplifier is used, R1 must be large enough so than not more than 500µA of current is drawn from the amplifier. R2 The value of R2 is determined from the mid-band gain of the error amplifier. This gain depends on the frequencies of the poles, zeros and LC filter resonant frequency. Based on the amount of gain necessary at the crossover frequency the mid-band gain and R2 value is calculated using the following formula. CO 2 CO G 1 R 2 R 1 fp 2 fz fz fc fc fo Vin H Vm G × = × ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ × ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ × × = The other component values are calculated as follows: 2 R 1 fz 2 1 2 C × × π × = 1 R 2 fz 2 1 3 C × × π × = ) 1 2 R 2 C 1 fp ( 2 2 C 3 C − × × × π × = 3 C 2 fp 2 1 3 R × × π × = Compensation of the Current Sharing Loop The control circuitry for Channel 2 forces the channel’s output current to match the current in Channel 1. The Channel 2 error amplifier compares the inductor currents in the two channels and adjusts the duty cycle of Channel 2 to control its output current. A block diagram is shown in Figure 27. |
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