Biomedical Engineering Reference
In-Depth Information
On-Body High Rate Line-of-Sight Communication
Let us consider the scenario shown in Fig. 2 a. The radio communication occurs
within a maximum of 2 m (i.e., a reasonable maximum distance between devices)
around the human body.
The literature reports 60-GHz wearable textile antennas with antenna gain ( G ANT )
of 12 dB [ 30 ].
As for the achievable performance of millimetre-wave CMOS transceiver, Chen
and Niknejad [ 31 ] report a 60 GHz power amplifier with 1-dB output, compression
point higher than 15 dBm, and Mitomo et al. [ 32 ] report a complete receiver with a
total NF of 14 dB.
Thus, consider a CMOS transceiver with the following performance, achievable
with modern nano-scale CMOS technologies:
• transmitted power P TX equal to 15 dBm
• receiver NF equal to 14 dB
• signal bandwidth equal to 1.76 GHz centered at 60 GHz.
Then, the receiver sensitivity ( S ) amounts to:
S
=−
174 dBm / Hz
+
NF
+
10
×
log 10 ( BW )
+
SNR
=−
50 dBm
(1)
The free space path loss ( PL ) amounts to:
log 10 λ (4 πd )
PL
=
20
×
=
74 dB
(2)
10 8
where λ
2m.
In the case of LOS communication, the received power ( P RX ) is equal to:
=
f / c
=
5mm( f
=
60 GHz, c
=
3
×
m/s) and d
=
P RX =
P TX +
2
×
G ANT
PL
=−
35 dBm
(3)
Thus, the loss margin ( LM ) left for shadowing, body loss, polarization mismatch,
and other losses, is equal to:
LM
=
P RX
S
=
15 dB
(4)
On-Body High Rate Nonline-of-Sight Communication
In the previous section, we considered on-body LOS communication. In spite of this,
the case offers an opportunity to derive some considerations, this communication
scenario is quite unrealistic since the position of each on-body transceiver relative
to the others varies as a consequence of the human body movements. Therefore, a
more appropriate scenario would be to consider the case in which omni-directional
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