Semiconductor devices - Semiconductor interface for human body communication - Part 2: Characterization of interfacing performances

IEC 62779-2:2016 defines a measurement method on electrical performances of an electrode that composes a semiconductor interface for human body communication (HBC). In the measurement method, a signal transmitter is electrically isolated from a signal receiver, so an isolation condition between the transmitter and receiver is maintained to accurately measure the electrode's performances. This part includes general and functional specifications of the measurement method.

Dispositifs à semiconducteurs - Interface à semiconducteurs pour les communications via le corps humain - Partie 2: Caractérisation des performances d'interfaçage

L'IEC 62779-2:2016 définit une méthode de mesure des performances électriques d'une électrode qui constitue une interface à semiconducteurs pour les communications via le corps humain. Dans la méthode de mesure, un émetteur de signaux est isolé électriquement d'un récepteur de signaux. Ceci assure le maintien de l'isolation entre l'émetteur et le récepteur pour mesurer avec exactitude les performances d'une électrode. La présente partie inclut des spécifications générales et fonctionnelles de la méthode de mesure.

General Information

Status
Published
Publication Date
17-Feb-2016
Technical Committee
Drafting Committee
Current Stage
PPUB - Publication issued
Start Date
18-Feb-2016
Completion Date
15-Mar-2016
Ref Project
Standard
IEC 62779-2:2016 - Semiconductor devices - Semiconductor interface for human body communication - Part 2: Characterization of interfacing performances
English and French language
33 pages
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Standards Content (Sample)


IEC 62779-2 ®
Edition 1.0 2016-02
INTERNATIONAL
STANDARD
NORME
INTERNATIONALE
Semiconductor devices – Semiconductor interface for human body
communication –
Part 2: Characterization of interfacing performances

Dispositifs à semiconducteurs – Interface à semiconducteurs pour les
communications via le corps humain –
Partie 2: Caractérisation des performances d'interfaçage

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IEC 62779-2 ®
Edition 1.0 2016-02
INTERNATIONAL
STANDARD
NORME
INTERNATIONALE
Semiconductor devices – Semiconductor interface for human body

communication –
Part 2: Characterization of interfacing performances

Dispositifs à semiconducteurs – Interface à semiconducteurs pour les

communications via le corps humain –

Partie 2: Caractérisation des performances d'interfaçage

INTERNATIONAL
ELECTROTECHNICAL
COMMISSION
COMMISSION
ELECTROTECHNIQUE
INTERNATIONALE
ICS 31.080.01 ISBN 978-2-8322-3175-3

– 2 – IEC 62779-2:2016 © IEC 2016
CONTENTS
FOREWORD . 3
INTRODUCTION . 5
1 Scope . 6
2 Normative references. 6
3 Terms, definitions and letter symbols . 6
3.1 General terms . 6
3.2 Signal characteristics . 9
3.3 Letter symbols . 11
4 Measurement of electrical performances of electrode . 11
4.1 Measurement setup . 11
4.2 Measurement apparatus and signal specifications . 12
4.2.1 Transmitter and receiver module . 12
4.2.2 Synchronization module . 13
4.2.3 Measurement equipment . 13
4.2.4 Signal specifications . 13
4.3 Measurement procedure . 14
4.3.1 General . 14
4.3.2 Attachment of transmitter and receiver modules . 14
4.3.3 Transmission of pulse and synchronization signals . 14
4.3.4 Synchronization of measurement equipment . 14
4.3.5 Signal processing in receiver module . 14
4.3.6 Measurement of pulse and processed signal . 14
4.3.7 Compensation for signal processing . 14
4.3.8 Computation of impulse response and complex transfer function . 14
4.4 Post processing for electrode performances . 14
4.4.1 General . 14
4.4.2 In-band average signal-loss . 14
4.4.3 In-band average phase-shift . 15
4.4.4 RMS delay . 15
4.4.5 Coherent bandwidth . 15
Bibliography . 17

Figure 1 – Pulse signal . 8
Figure 2 – Synchronization signal . 9
Figure 3 – Measurement setup . 12

Table 1 – Letter symbols . 11

INTERNATIONAL ELECTROTECHNICAL COMMISSION
____________
SEMICONDUCTOR DEVICES – SEMICONDUCTOR INTERFACE
FOR HUMAN BODY COMMUNICATION –

Part 2: Characterization of interfacing performances

FOREWORD
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indispensable for the correct application of this publication.
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patent rights. IEC shall not be held responsible for identifying any or all such patent rights.
International Standard IEC 62779-2 has been prepared by IEC technical committee 47:
Semiconductor devices.
The text of this standard is based on the following documents:
FDIS Report on voting
47/2268/FDIS 47/2278/RVD
Full information on the voting for the approval of this standard can be found in the report on
voting indicated in the above table.
This publication has been drafted in accordance with the ISO/IEC Directives, Part 2.

– 4 – IEC 62779-2:2016 © IEC 2016
A list of all parts in the IEC 62779 series, published under the general title Semiconductor
devices – Semiconductor interface for human body communication, can be found on the IEC
website.
The committee has decided that the contents of this publication will remain unchanged until
the stability date indicated on the IEC web site under "http://webstore.iec.ch" in the data
related to the specific publication. At this date, the publication will be
• reconfirmed,
• withdrawn,
• replaced by a revised edition, or
• amended.
INTRODUCTION
The IEC 62779 series is composed of three parts as follow:
• IEC 62779-1 defines general requirements of a semiconductor interface for human body
communication. It includes general and functional specifications of the interface.
• IEC 62779-2 defines a measurement method on electrical performances of an electrode
that constructs a semiconductor interface for human body communication.
• IEC 62779-3 defines functional type of a semiconductor interface for human body
communication, and operational conditions of the interface.

– 6 – IEC 62779-2:2016 © IEC 2016
SEMICONDUCTOR DEVICES – SEMICONDUCTOR INTERFACE
FOR HUMAN BODY COMMUNICATION –

Part 2: Characterization of interfacing performances

1 Scope
This part of IEC 62779 defines a measurement method on electrical performances of an
electrode that composes a semiconductor interface for human body communication (HBC). In
the measurement method, a signal transmitter is electrically isolated from a signal receiver, so
an isolation condition between the transmitter and receiver is maintained to accurately
measure the electrode’s performances. This part includes general and functional
specifications of the measurement method.
HBC uses the body of a user as a transmission medium using near-field coupling inside the
body: a signal transmitter and receiver are coupled with each other through a near field that is
formed inside the human body and air. The intensity of the near field is strong especially
inside the body due to high dielectric constant of the body, so a data signal is transmitted
through the human body by modulating the near field. A signal transmitter and receiver for
HBC include an internal ground respectively, and, in most HBC applications, the grounds are
separated from each other as maintaining the coupling condition through the air. Quality of a
data transmission strongly depends on a coupling degree between the grounds; hence, it is
important to maintain the coupling degree between grounds of a signal transmitter and
receiver for an accurate measurement of the electrode’s performances. This part defines a
measurement method to measure electrical performances of an electrode while the coupling
degree between grounds of a signal transmitter and receiver is maintained.
NOTE 1 HBC semiconductor interface consists of an electrode and analog front end.
NOTE 2 General analog and digital modulation techniques can be used to modulate a near field used in HBC, and
a modulation technique to be used is determined according to required performances for a data transmission and a
HBC application.
2 Normative references
The following referenced documents are indispensable for the application of this document.
For dated references, only the edition cited applies. For undated references, the latest edition
of the referenced document (including any amendments) applies.
None.
3 Terms, definitions and letter symbols
For the purposes of this document, the following terms and definitions apply.
3.1 General terms
3.1.1
electrode
physical structure to transmit an electrical signal between an analog front end and the human
body while attached to or located near the human body
Note 1 to entry: An electrode transfers an electrical signal to be transmitted to a non-metallic transmission
channel, the human body. It also transfers an electrical signal received from the human body to the analog front
end.
Note 2 to entry: electrode can have an adhesive material on its surface like a disposable ECG electrode to be
attached itself to the human body; or a metal surface for a simple implementation. In the case of a metal surface,
an electrode makes contact with the human body by attaching it to the human body using an attachment aid like a
rubber band; or simply touching it with the hand.
[SOURCE: IEC 62779-1: 3.1.1, modified – Note 2 to entry has been added.]
3.1.2
transmitter module
circuit module that generates a pulse signal to be transmitted to the human body through an
electrode for measurement of the electrode’s performances; and a synchronization signal of
an optical type to be transmitted through an optical cable for synchronization of the pulse
signal transmitted through the human body
Note 1 to entry: A transmitter module includes a signal amplifier to amplify the transmitting pulse signal; and a
signal filter to remove a signal component causing an interference to other measurement modules and
measurement equipment.
3.1.3
receiver module
circuit module that processes a pulse signal received from the human body through an
electrode to increase signal quality for measurement of the electrode’s performances
Note 1 to entry: A receiver module includes a signal amplifier to amplify the received pulse signal; and a signal
filter to remove a noise or interference signal from the received pulse signal.
3.1.4
synchronization module
circuit module that transforms a synchronization signal transmitted through an optical cable
into an electrical signal; and generates a trigger signal using the transformed synchronization
signal to trigger measurement equipment
Note 1 to entry: A synchronization module includes an optical transceiver to transform an optical signal into an
electrical signal or vice versa.
3.1.5
pulse signal
electrical signal that is generated in the transmitter module and then transmitted to the human
body through an electrode to measure the electrode’s performances while having a specific
pulse-width to include a signal component at frequency bands over which the performances
are to be measured
Note 1 to entry: Figure 1 shows a pulse signal and its related terms.

– 8 – IEC 62779-2:2016 © IEC 2016
PP
P
PA
P
Time
RT
P
FT
P
PA
P
0,9PA
P
STF
P
0,1PA
P
PW
P
Time
IEC
Key
PA Pulse amplitude PP Pulse period
p p
US Undershoot PW Pulse width
p p
RT FT
Rising time Falling time
p p
STF Settling time of falling
p
Figure 1 – Pulse signal
Note 2 to entry: A pulse signal has a short pulse-width to include a signal component at a wide-frequency band.
3.1.6
synchronization signal
electrical signal that is synchronized to the pulse signal and then transformed into an optical
signal to be transmitted to a synchronization module through an optical cable for the purpose
of synchronization between the transmitter and receiver modules
Note 1 to entry: Figure 2 shows a synchronization signal and its related terms.
Amplitude
Amplitude
US
P
PA
S
US
S
Time
RT FT
S S
1,1 PA
S
PA
S
0,9PA
S
STR STF
S S
0,1PA
S
–0,1PA PW
S S
Time
IEC
Key
PA Pulse amplitude OS overshoot
s s
US Undershoot PW Pulse width
s s
RT FT
Rising time Falling time
s s
STR Settling time of rising STF Settling time of falling
s s
Figure 2 – Synchronization signal
3.2 Signal characteristics
3.2.1
pulse amplitude
PA
p
peak amplitude of pulse signal in volts
3.2.2
pulse period
PP
p
time period of periodic pulses in seconds
3.2.3
undershoot
US
p
minimum amplitude in volts during transient period of a falling signal
Amplitude
Amplitude
OS
S
– 10 – IEC 62779-2:2016 © IEC 2016
3.2.4
pulse width
PW
p
time interval in seconds between points at which a pulse signal has 10 % value of pulse
amplitude
3.2.5
rising time
RT
p
time interval in seconds required for a pulse signal to rise from 10 % value of pulse amplitude
to 90 % value
3.2.6
falling time
FT
p
time interval in seconds required for a pulse signal to fall from 90 % value of pulse amplitude
to 10 % value
3.2.7
settling time of falling
STF
p
maximum time interval in seconds required for a pulse signal to fall from 90 % value of pulse
amplitude to 10 % or −10 % value during transient period of a falling signal
3.2.8
pulse amplitude
PA
s
peak amplitude of a synchronization signal in volts after transient period of a rising signal
3.2.9
overshoot
OS
s
differential amplitude in volts from pulse amplitude to peak amplitude during transient period
of a rising signal
3.2.10
undershoot
US
s
minimum amplitude in volts during transient period of a falling signal
3.2.11
pulse width
PW
s
time interval in seconds between points at which a synchronization signal has 10 % value of
pulse amplitude
3.2.12
rising time
RT
s
time interval in seconds required for a synchronization signal to rise from 10 % value of pulse
amplitude to 90 % value
3.2.13
falling time
FT
s
time interval in seconds required for a synchronization signal to fall from 90 % value of pulse
amplitude to 10 % value
3.2.14
settling time of rising
STR
s
maximum time interval in seconds required for a synchronization signal to rise from 10 %
value of pulse amplitude to 110 % or 90 % value during transient period of a rising signal
3.2.15
settling time of falling
STF
s
maximum time interval in seconds required for a synchronization signal to fall from 90 % value
of pulse amplitude to 10 % or −10 % value during transient period of a falling signal
3.3 Letter symbols
For the purposes of this document, the letter symbols given in Table 1 apply.
Table 1 – Letter symbols
Name and designation Letter symbol
PA
Pulse amplitude
p
Pulse period PP
p
Undershoot US
p
Pulse width PW
p
Rising time RT
p
Falling time FT
p
Settling time of falling STF
p
PA
Pulse amplitude
s
Overshoot OS
s
Undershoot US
s
Pulse width PW
s
Rising time RT
s
Falling time FT
s
Settling time of rising STR
s
Settling time of falling STF
s
4 Measurement of electrical performances of electrode
4.1 Measurement setup
A measurement setup as shown in Figure 3 is applied to measure interface performances
while maintaining a coupling degree between grounds inside a signal transmitter and receiver.

– 12 – IEC 62779-2:2016 © IEC 2016
Pulse signal Receiving signal
SP
t t
TM RM
Measurement
equipment
ET ET
Sync. signal Trigger signal
t t
SM
OC
IEC
Key
TM Transmitter module RM Receiver module
SM Synchronization module OC Optical cable
SP Signal probe ET Electrode
Figure 3 – Measurement setup
4.2 Measurement apparatus and signal specifications
4.2.1 Transmitter and receiver module
4.2.1.1 General
For an accurate measurement of the electrode’s performances, physical and electrical
specifications of the modules are determined as follows.
4.2.1.2 Size of internal ground plane
An internal ground plane inside a transmitter and receiver module shall have the same size as
that of a device to which a HBC semiconductor interface is applied.
4.2.1.3 Amplitude of pulse signal
A pulse signal transmitted through an electrode to the human body shall have enough small
amplitude to minimize any potential harmful health effects that may occur during transmitting
the pulse signal.
If applicable, general regulations to limit human exposure to electromagnetic fields (EMF)
shall be satisfied.
4.2.1.4 Interface
Each module shall include an interface for a measurement equipment to measure a pulse
signal in the transmitter module and a processed signal in the receiver module.
4.2.1.5 Modulation technique
In the transmitter, any modulation technique can be used to transform a synchronization
signal to an optical signal transmitted through an optical cable.

4.2.2 Synchronization module
4.2.2.1 General
A synchronization module shall be sufficiently distant from the human body to avoid signal
interference with a pulse signal transmitted through the human body.
4.2.2.2 Demodulation technique
A demodulation technique corresponding to the modulation technique used for a
synchronization signal shall be used to transform an optical signal received through an optical
cable to a synchronization signal.
4.2.3 Measurement equipment
Measurement equipment including a signal probe shall be prepared to measure a pulse signal
in the transmitter module and a processed signal in the receiver module respectively.
The measurement equipment shall be synchronized with the pulse signal in transmitter using
a trigger signal generated from the synchronization module.
4.2.4 Signal specifications
4.2.4.1 General
The following specifications of the signals that are used for measurement shall be given.
4.2.4.2 Pulse signal
The following specifications of the pulse signal shall be given:
a) pulse amplitude;
b) pulse period;
c) undershoot;
d) pulse width;
e) rising time;
f) falling time;
g) settling time of falling.
4.2.4.3 Synchronization signal
The following specifications of the synchronization signal shall be given:
a) pulse amplitude;
b) overshoot;
c) undershoot;
d) pulse width;
e) rising time;
f) falling time;
g) settling time of rising;
h) settling time of falling.
– 14 – IEC 62779-2:2016 © IEC 2016
4.3 Measurement procedure
4.3.1 General
The interface performance is measured according to the following procedure.
4.3.2 Attachment of transmitter and receiver modules
A transmitter and a receiver module, each having an electrode under measurement, are
attached to the human body.
4.3.3 Transmission of pulse and synchronization signals
A pulse signal that is generated in a transmitter module is transmitted to the human body
through the electrode. Furthermore, a synchronization signal that is synchronized to the pulse
signal is transmitted to an optical cable for synchronization after being transformed into an
optical signal.
4.3.4 Synchronization of measurement equipment
A synchronization module transforms an optical signal transmitted through an optical cable
into a synchronization signal; it then generates a trigger signal to synchronize a measurement
equipment to a pulse signal in a transmitter module.
4.3.5 Signal processing in receiver module
A receiving signal is processed in a receiver module. The signal processing includes signal
amplification and filtering.
4.3.6 Measurement of pulse and processed signal
A pulse signal in a transmitter module is measured using a signal probe in the measurement
equipment; then a processed signal in a receiver module is measured using the same signal
probe while synchronization with a pulse signal in a transmitter module is maintained.
4.3.7 Compensation for signal processing
An amplitude gain by signal processing in a receiver module is compensated to obtain a
receiving signal received at an electrode of the receiver module.
4.3.8 Computation of impulse response and complex transfer function
After pulse and receiving signals are respectively transformed into the frequency domain, the
transformed receiving signal is subtracted from the transformed pulse signal to obtain a
complex transfer function. An impulse response is obtained by transforming the obtained
complex transfer function into the time domain.
4.4 Post processing for electrode performances
4.4.1 General
After obtaining an impulse response, h[n], and complex transfer function, H[m], from the
comparison of the pulse and receiving signals, electrical performances shall be calculated as
follows.
4.4.2 In-band average signal-loss
The in-band average signal-loss can be calculated from the complex transfer function as
follows:
M
[ ]
SL = H m (1)

average
M −M +1
m=M
1 2
Here, SL is the in-band average signal loss, and H[m] is the complex transfer function
average
with a frequency index m. M and M represent the frequency band where the signal loss is
1 2
averaged.
4.4.3 In-band average phase-shift
The in-band average phase-shift can be calculated from the complex transfer function as
follows:
M
PS = ∠H[m] (2)

average
M −M +1
m=M
1 2
Here, PS is the in-band average phase-shift.
average
4.4.4 RMS delay
The RMS delay can be calculated from a power de
...

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