Rainbow Electronics MAX1801 User Manual

Page 12

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MAX1801

Digital Camera Step-Up Slave
DC-DC Controller

12

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1) Choose the compensation resistor R

C

that is equiv-

alent to the inverse of the transconductance of the
error amplifier, 1/ R

C

= G

EA

= 100µS, or R

C

= 10k

Ω.

This sets the high-frequency voltage gain of the
error amplifier to 0dB.

2) Determine the maximum output pole frequency:

where:

R

LOAD(MIN)

= V

OUT

/ I

OUT(MAX)

3) Place the compensation zero at the same frequency

as the maximum output pole frequency (in Hz):

Solving for C

C

:

Use values of C

C

less than 10nF. If the above calcu-

lation determines that the capacitor should be
greater than 10nF, use C

C

= 10nF, skip step 4 , and

proceed to step 5.

4) Determine the crossover frequency (in Hz):

f

C

= V

REF

/ (

π

D C

OUT

)

and to maintain at least a 10dB gain margin, make
sure that the crossover frequency is less than or
equal to 1/3 of the ESR zero frequency, or:

3f

C

≤ Z

O

or:

ESR

≤ D / 6 V

REF

If this is not the case, go to step 5 to reduce the
error amplifier high-frequency gain to decrease the
crossover frequency.

5) The high-frequency gain may be reduced, thus

reducing the crossover frequency, as long as the
zero due to the compensation network remains at or
below the crossover frequency. In this case:

ESR

≤ D / (G

EA

R

C

6 V

REF

)

and:

f

C

= (G

EA

R

C

) 2 V

REF

/ (2

π

D C

OUT

)

≥ 1 / (2

π

R

C

C

C

)

Choose C

OUT

, R

C

, and C

C

to simultaneously satisfy

both equations.

Continuous Inductor Current

For continuous inductor current, there are two condi-
tions that change, requiring different compensation.
The response of the control loop includes a right-half-
plane zero and a complex pole pair due to the inductor
and output capacitor. For stable operation, the con-
troller loop gain must drop below unity (0dB) at a much
lower frequency than the right-half-plane zero frequen-
cy. The zero arising from the ESR of the output capaci-
tor is typically used to compensate the control circuit
by increasing the phase near the crossover frequency,
increasing the phase margin. If a low-value, low-ESR
output capacitor (such as a ceramic capacitor) is used,
the ESR-related zero occurs at too high a frequency
and does not increase the phase margin. In this case,
use a lower value inductor so that it operates with dis-
continuous current (see the Discontinuous Inductor
Current
section).

For continuous inductor current, the gain of the voltage
divider is A

VDV

= V

REF

/ V

OUT

, and the DC gain of the

error amplifier is A

VEA

= 2000. The gain through the

PWM controller in continuous current is:

A

VO

= (1 / V

REF

) (V

OUT2

/ V

IN

)

Thus, the total DC loop gain is:

A

VDC

= 2000 V

OUT

/ V

IN

The complex pole pair due to the inductor and output
capacitor occurs at the frequency (in Hz):

P

O

= (V

OUT

/ V

IN

) / (2

π

(L

× C

OUT

)

1/2

)

The pole and zero due to the compensation network at
COMP occur at the frequencies (in Hz):

P

C

= G

EA

/ (4000

π

C

C

) = 1 / (4 x 10

7

π

C

C

)

Z

C

= 1 / (2

π

R

C

C

C

)

The frequency (in Hz) of the zero due to the ESR of the
output capacitor is:

Z

O

= 1 / (2

π

C

OUT

ESR)

And the right-half-plane zero frequency (in Hz) is:

The Bode plot of the loop gain of this control circuit is
shown in Figure 5.

Z

(1 - D) R

2 L

RHP

2

LOAD

=

π

C

C

V

V

- V

I

V

- V

C

OUT OUT

OUT

IN

C OUT(MAX)

OUT

IN

=

R

(

)

2

Z

1

2V

- V

V

- V

C

C

C C

OUT

IN

OUT

IN

LOAD(MIN)

OUT

=

=

2

2

π

π

R C

R

(

)

P

2V

- V

V

- V

C

O(MAX)

IN

IN

LOAD(MIN)

=

OUT

OUT

OUT

R

2

π(

)

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