7 valley switching, Cs1501, Zcd_below _zero – Cirrus Logic CS1501 User Manual

Page 11

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background image

CS1501

DS927F4

11

Resistor R

IFB

sets the feedback current and is calculated as

follows:

By using digital loop compensation, the voltage feedback
signal does not require an external compensation network.
A current proportional to the AC input voltage is supplied to the
IC on pin IAC and is used by the PFC control algorithm.

Figure 17. IAC Input Pin Model

Resistor R

IAC

sets the I

AC

current and is derived as follows:

For optimal performance, resistors R

IAC

and R

IFB

should use

1% tolerance or better resistors for best V

link

voltage accuracy.

5.7 Valley Switching

The zero-current detection (ZCD) pin is monitored for
demagnetization in the auxiliary winding of the boost inductor
(L

B

). The ZCD circuit is designed to detect the V

Aux

valley/zero crossings by sensing the voltage transformed onto
the auxiliary winding of L

B

.

Figure 18. ZCD Input Pin Model

The objective of zero-voltage switching is to initiate each

MOSFET switching cycle when its drain-source voltage is at
the lowest possible voltage potential, thus reducing switching
losses. The CS1501 uses an auxiliary winding on the PFC
boost inductor to implement zero-voltage switching.

Figure 19. Zero-voltage Switch

During each switching cycle, when the boost diode current
reaches zero, the boost MOSFET drain-source voltage begins
oscillating at the resonant frequency of the boost inductor and
MOSFET parasitic output capacitance. The ZCD_below_zero
signal transitions from high to low just prior to a local minimum
of the MOSFET drain-source voltage oscillation. The
zero-crossing detect circuit ensures that a ZCD_below_zero
pulse will only be generated when the comparator output is
continuously high for a nominal time period (t

ZCB

) of 200ns.

Therefore, any negative edges on the comparator's output
due to spurious glitches will not cause a pulse to be
generated. Due to the CS1501’s variable-frequency control,
the MOSFET switching cycle will not always be initiated at the
first resonant valley.
The external circuitry should be designed so that the current
(I

ZCD

) at the ZCD pin is approximately

1.0 mA. The table

below depicts approximate values for R3 and R4 for a range
of boost-to-auxiliary inductor turns ratio, N.

Table 1. Aux Inductor Turns Ratio vs. R3 and R4

Resistors R3 and R4 were calculated using V

link

= 400V and

C

p

= 10pF.

Equation 6 is used to calculate the cut-off frequency defined
by the RC circuit at the ZCD pin.

where:
f

c

The cut-off frequency, f

c

, needs to be 10x the ringing

frequency

C

p

Capacitance at the ZCD pin

R

IFB

V

link

V

DD

I

ref

-----------------------------

400V V

DD

129

A

-------------------------------

=

=

[Eq.4]

R1

R

IAC

I

AC

IA C

V DD

15k

8

V

rect

CS1501

24k

ADC

R2

3

I

ref

R

IAC

R

IFB

=

[Eq.5]

R3

I

Aux

V

link

ZCD

L

B

R4

CS1501

ZCD_below_zero

D2

FE T Drain

N:1

+

V

Aux

-

Demag

Comparator

+

-

V

th( Z CD)

5

I

Z CD

C

p

N

~R3

~R4

9

46k

1.75k

10

42k

1.75k

11

37.5k

1.75k

12

35.5k

1.75k

13

32k

1.75k

14

29.5k

1.75k

15

27.5k

1.75k

ZCD

Zero Crossing

Detection

GD ‘ON’

ZCD_below _zero

f

c

1 2

 R3 R4



C

p

=

[Eq.6]

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