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Common-mode transient rejection, Introduction – Avago Technologies ACPL-224-500E User Manual

Page 6

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AV02-4387EN

4

Avago Technologies

Figure 5. Illustration of V

CM

Common-Mode Pulse.

Figure 6a. Interference Circuit Model.

Circuit designers often encounter

the adverse effects of common-

mode noise in a design. Once a

common-mode problem is identi-

fied, there are several ways that it

can be resolved. However, common-

mode interference manifests itself in

many ways; therefore, it may be hard

to determine whether it is the cause

of a circuit’s misbehavior. If a system

is connected and running but only

produces erroneous data, common-

mode noise may be the reason.

This section describes sources of

common-mode problems, presents

possible solutions, and highlights

the technology that Avago Tech-

nologies' Components Group uses

to produce opto-isolators with su-

perior Common-Mode Performance.
Common-mode rejection (CMR) is

a measure of the ability of a device

to tolerate common-mode noise.

Avago specifies common-mode

rejection as common-mode transient

rejection (CMTR). CMTR describes the

maximum tolerable rate-of-rise (or

fall) of a common-mode voltage

(given in volts per micro second). The

specification for CMTR also includes

the amplitude of the common-mode

voltage (V

CM

) that can be tolerated.

Common-mode interference that

exceeds the maximum specifica tion

might result in abnormal voltage

transitions or excessive noise on the

output signal. (CMTR is slightly dif-

ferent than common-mode rejec-

tion ratio CMRR, often used for analog

devices and commonly specified in

dB as the ratio of the differential-

mode gain to the common-mode

gain.)
Avago optocouplers rely on two

key technical strengths to achieve

high CMTR. The first is use of a pro-

prietary, low-cost Faraday shield

which decouples the optocoupler

input side from the output side.

The second method is by unique

package design which minimizes

input-to-output capacitance. The

importance of these two strengths is

explained as follows.
Figure 5 illustrates a Common-mode

transient pulse (V

CM

).

Figure 6a and 6b show interfer-

ence circuit models for two types

of possible common-mode failure

mechanisms for a single-transistor

optocoupler. The dashed lines are

shown to indicate external compo-

nents added to the optocoupler. V

CM

represents a voltage spike across the

optocoupler isolation path between

the output-side ground (V

G2

) and

input-side ground (V

G1

). V

DM

repre-

sents a signal voltage applied across

the input side.

R

L

+ (V

CM

)

OPTO-

ISOLATOR

COMMON-MODE TRANSIENT

R

V

TRANSMIT SIDE

RECEIVE SIDE

VOLTMETER

LED

V

DM

V

G1

INPUT GROUND

V

G2

OUTPUT GROUND

C

SB

C

IS

i

CM

I

B

I

P

PHOTODIODE

V

O

R

L

INTERNAL SHIELD

NOTE: i

CM

GETS DIVERTED TO GROUND, V

G2

, WHEN INPUT IS OFF.

i

CM

IS SUPPLIED FROM GROUND, V

G2

, WHEN OUTPUT IS ON.

V

CM

VOLTMETER

Common-Mode Transient Rejection

Introduction

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