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BRIEF COMMUNICATION
Interface of data transmission for a transcutaneouscommunication system using the human body as transmissionmedium
Eiji Okamoto • Yoshikuni Kato • Kazuyuki Seino •
Yoshinori Mitamura
Received: 14 January 2011 / Accepted: 2 August 2011 / Published online: 21 August 2011
� The Japanese Society for Artificial Organs 2011
Abstract We have been developing a new transcutaneous
communication system (TCS) that uses the human body as
an electrical conductive medium. We studied an interface
circuit of the TCS in order to optimize the leading data
current into the human body effectively. Two types of LC
circuits were examined for the interface circuit, one was an
LC series-parallel circuit, and the other was a parallel-
connected LC circuit. The LC series-parallel circuit con-
nected to the body could be tuned to a resonant frequency,
and the frequency was determined by the values of an
external inductor and an external capacitor. Permittivity of
the body did not influence the electrical resonance. Con-
nection of the LC series-parallel circuit to the body
degraded the quality factor Q because of the conductivity
of the body. However, the LC parallel-connected circuit
when connected to the body did not indicate electrical
resonance. The LC series-parallel circuit restricts a direct
current and a low-frequency current to flow into the body;
thus, it can prevent a patient from getting a shock.
According to the above results, an LC series-parallel circuit
is an optimum interface circuit between the TCS and the
body for leading data current into the body effectively and
safely.
Keywords Artificial heart � Intra-body communication �Transcutaneous data communication � Monitoring
Introduction
A transcutaneous communication system (TCS) is one of
the key technologies for monitoring and controlling artifi-
cial hearts and other artificial organs that are implanted
inside the body. The TCS needs to have stable bi-direc-
tional communication through the skin without interference
from other patient devices.
Intra-body communication using a human body as a
transmission conductor has been investigated in order to
achieve personal networks for communication between
wearable information devices and sensors [1–3].
We have been developing a new TCS that uses the
intra-body communication technology [4]. The new TCS
was able to transmit data concurrently and bi-direc-
tionally on the surface of a human body under full
duplex communication at a transmission rate of
115 kbps. The performance of the TCS is superior not
only to that of the traditional transcutaneous information
systems using electromagnetic or optical data transmis-
sion, but also to the reported intra-body communication
systems [5–7].
The electrical properties of the body are represented by
an equivalent circuit with resistors and capacitors. In a
previous study, we could obtain an electrical resonance
while leading ASK-modulated current into a human body
through an inductor. However, the mechanism of an L–C
resonance incorporating the human body has not been
studied. Hwang et al. already reported the design of a
data-receiving circuit of intra-body communication [8],
but an optimal interface for data transmission has not been
found.
In this study, we studied an interface of the TCS with a
human body in order to understand the electrical properties
of the human body when leading a data current and in order
E. Okamoto (&) � Y. Kato � K. Seino � Y. Mitamura
Department of Human Science and Informatics,
School of Biological Science and Engineering,
Tokai University, 5-1-1-1 Minami-sawa,
Minami-ku, Sapporo, Japan
e-mail: [email protected]
123
J Artif Organs (2012) 15:99–103
DOI 10.1007/s10047-011-0600-x
to optimize the interface circuit for data output into the
human body.
The aim of this article was to study an interface circuit
of the TCS in order to achieve a suitable interface circuit
with the human body for stable and efficient data
transmission.
Method
A TCS has an external and an internal unit, and each unit
consists mainly of a data transmitter and a data receiver
[4]. The data transmitter has an oscillator (carrier fre-
quency: 4 and 10 MHz), an amplitude shift keying (ASK)
modulator, and Ag–AgCl electrodes. The ASK-modulated
data current is led into a human body through a trans-
former, and it flows back to the ground terminal of an
energy source through the body, space around the patient
and a data receiver. The data receiver consists of an Ag–
AgCl electrode, an LC parallel-tuned circuit, and an ASK
demodulator.
In this study, two types of LC circuits were examined
as data transmission interface: one was an LC series-par-
allel circuit in which an inductor was connected in parallel
with series-connected capacitors, and the other was a
parallel-connected LC circuit. A junction node between
the capacitors in the LC series-parallel circuit was con-
nected to the left forearm of a subject through an ECG
Ag–AgCl electrode [Life Med Co., Soft-E S30/A (L),
Tokyo, Japan] removing conductive paste spread on the
contact interface, and alternate current was led into the
human body. Voltage on the transmission electrode was
measured by an oscilloscope (TTF Co., Tektronix MSO
4032, Tokyo, Japan) using a high-input impedance FET
probe (TTF Co., Tektronix p6243, Tokyo, Japan) to
evaluate frequency characteristics under changing capaci-
tance of the capacitors.
The parallel-connected LC circuit was also connected to
a human body in parallel through an Ag–AgCl electrode,
and frequency characteristics were also measured.
All procedures in this study were approved by the Tokai
University institutional review board for human research.
Results
Figure 1a shows tuning characteristics of the LC series-
parallel circuit at a carrier frequency of 4 MHz. Two
capacitors having the same capacitance (C1 = C2) were
connected in series, and three kinds of voltage were
measured under changing capacitance of both capacitors.
The terminal voltage of an inductor under connecting
capacitors to the body Vo2 showed characteristics of a
parallel resonance circuit like the voltage Vo1, and the
voltage on an electrode Vo3, which was the node voltage
of the series-connected capacitors, also showed a resonant
characteristic.
Figure 1b shows tuning characteristics of an LC paral-
lel-connected circuit at a carrier frequency of 4 MHz. The
terminal voltage of the LC parallel-connected circuit Vo1
showed resonant characteristics like the LC series-parallel
circuit in Fig. 1a. However, the terminal voltage of the LC
parallel-connected circuit connected to the body Vo2 did
not show resonance, and the amplitude change of the
voltage Vo2 was quite small under changing capacitance of
the tuning capacity.
From the above results, the LC series-parallel circuit is
suitable for an interface circuit of a TCS to lead commu-
nication data current effectively into the body.
Discussion
We have been developing a TCS for communication
between a host monitor outside the body and an internal
artificial heart controller inside the body using the body as
a transmission conductor. In general, the electrical char-
acteristics of tissue are determined by their conductivity
and permittivity depending on current frequency, and the
electrical properties of the body as an assembly of tissue
are represented by an equivalent circuit consisting of
resistors and capacitors.
In a previous study, we examined a series-connected LC
interface circuit connected to a human body. Development
of electrical resonance depended on the length of the signal
line, and installation of a capacitor between the signal line
and a circuit ground made a stable electrical resonance
regardless of the length of the signal line [9].
Leading current into the body under electrical reso-
nance has several advantages: effective application of
transmission current, and band limitation of the transmis-
sion current contributing to both bi-directional communi-
cation and protection against shock caused by low
frequency currents.
However, the mechanism of electrical resonance when
connecting the LC interface circuit to the human body has
not been determined. Also an optimum design of the LC
interface circuit between the TCS and the body have not
been reported. Therefore, in this article, we studied the LC
interface circuit in order to clarify the effect of the elec-
trical properties of the body on the LC electrical resonance
in order to achieve an optimum interface circuit for data
transmission.
An LC series-parallel circuit connected to a human
body showed electrical resonance (Fig. 1a). Capacitances
of the tuning capacity at resonance were the same in
100 J Artif Organs (2012) 15:99–103
123
terminal voltages Vo1, Vo2, and Vo3; thus, permittivity of
the body did not influence electrical resonance. However,
an LC parallel-connected circuit connected to the body did
not indicate electrical resonance, as shown in Fig. 1b.
The body is electrically represented by an RC parallel
circuit, as shown Fig. 2a, and the LC series-parallel circuit
connected to the body is electrically expressed as in
Fig. 2b. When the capacitance of a capacitor originated
from permittivity of the body, C3 was much smaller than
the capacitance of an external capacitor C2; an equivalent
circuit of the LC series-parallel circuit connecting to the
body is simplified in Fig. 2c. The resonant frequency fr is
determined by the inductor L and the external capacitor C1,
C2, and it is expressed as follows,
fr ¼ 1
2pffiffiffiffiffiffi
LCp ð1Þ
where
C ¼ C1 � C2
C1 þ C2
ð2Þ
Capacitor components of the body C3 are not included in
resonant frequency fr; thus, the size of the human body
does not affect resonant frequency.
The quality factor Q is a measure of the quality of a
tuned circuit, and it is determined by a ratio of resonant
frequency to the bandwidth of the tuned circuit. As shown
in Fig. 1a, the quality factor Q of the LC series-parallel
circuit decreased from Vo1 to Vo3 by connecting to the
body. The quality factor Q of the tuned circuit is also given
by the ratio of susceptance to its conductance. Therefore,
connection of the LC series-parallel circuit to the body
degrades the quality factor Q because of the increase in
conductance by adding the conductivity of the body.
As for the LC parallel-connected circuit, an increase of
conductivity by connecting to the body decreases the
quality factor Q greatly, and it causes disappearance of
0
1
2
3
4
5
6
7
8
0 50 100 150 200 250
Tuning Capacitance C (pF)
Vou
t (V
)
21
21
CC
CCC= =
+C21C C
0
1
2
3
4
5
6
7
8
9
0 50 100 150 200 250
Vou
t(V
)
Tuning Capacitance C(pF)
4MHz
4MHz
(a)
(b)
Fig. 1 Frequency
characteristics of the interface
circuit for leading data current
into the body. a The LC series-
parallel circuit connected to the
body. b The LC parallel
connected circuit connected to
the body
J Artif Organs (2012) 15:99–103 101
123
electric resonance when connecting the LC parallel-con-
nected circuit to the body (Fig. 1b).
The LC series-parallel circuit applied for a data trans-
mission interface to the body has another advantage. Both a
transformer used as an inductor L and a capacitor C1,
which is connected in series between the transformer and
the body, restrict a direct current and a low-frequency
current to flow into the body, and it prevents a patient from
getting a shock.
From the above results, the series-parallel LC circuit
shown in Fig. 1a is a suitable interface circuit for leading
current into a human body effectively and safely.
Further study is required to evaluate the performance
of the TCS interface circuit under transcutaneous bi-
directional data transmission in a long-term animal
experiment.
Conclusion
We have studied an interface circuit of the TCS using a
human body as electrical conductive medium. An LC
series-parallel circuit is an optimum interface between the
electronics of the TCS and the human body for leading data
transmission current into the human body effectively and
safely, and it should promise stable communication
between an implanted artificial organ and external monitor
outside the body.
Acknowledgments This study was supported by KAKENHI
[Grant-in-Aid for Scientific Research-C (22500413), 2010] and the
program for Promotion of Fundamental Studies of the Tateishi Sci-
ence and Technology Foundation, 1091004, 2009.
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LC
1
2=
+=
21
21
CC
CCC
(a)
(b)(c)
Fig. 2 Equivalent circuit of
interface for leading data
current into the body
102 J Artif Organs (2012) 15:99–103
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