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WELL COME
TO OUR
PRESENTATION
Presentation
On
“An Ultra-Wideband Wire Spiral
Antenna for In-Body Communications
Using Different Material Matching
Layers.”
Author By
• Ali Khaleghi
• Ilangko Balasingham and
• Raúl Chávez-Santiago
Presented TO
Md. Imran Khan
Lecturer
Dept. Of Electrical and Electronic Engineering
World University Of Bangladesh
Presented By
Abdul Kader
Id No: WUB 09/13/52/2102
&
Md. Rabiul Alam Sourav
Id No: WUB 09/13/52/2091
Contents
• Abstract
• Introduction
• Antenna Design
• Measured and simulated return loss
• Gain Vs Frequency
• Measured and simulated radiation pattern for the E-
plane and H-plane
• Return loss versus frequency for different material
• Scenario of the spiral antenna near an anatomical
model
Abstract
1. Used for getting information from human
body.
2. Operating frequency 3-10 GHz and
impedance 200 ohm in free space and
permittivity values ranging from 12-74.
3. The best improvement in wave penetration
was obtained for the frequency is 750-1000
MHz and inside material permittivity is 27.
Introduction
• This compact antenna is required for a number of
diagnostic and therapeutic applications.
• A properly designed antenna can transmit /receive
to/from an implanted device over a significant part of the
radio spectrum or transfer electromagnetic (EM) energy
to internal organs.
• The main problem in these applications is suffered in
biological tissues.
Introduction
• The proposed antenna design has an impedance of 30-60 Ω .
(according to material)
• Example: When embedded in distilled water with permittivity
equal to 74, the antenna covers the frequency range of 300-
1000 MHz.
Ultra wide Band
USES:
UWB has several potential applications in
medicine. Other uses are:
Increasing data rate , a microwave
hyperthermia applicator , microwave imaging
radar etc.
Antenna Design
Fig. 1. Dual Spiral Archimedes
antenna on top of a ground plane Fig. 2. Photography of the fabricated
antenna and the matching unit.
Fig. 3. Antenna impedance versus frequency in free space.
Most wireless implantable medical devices
operate in the narrowband frequency band of
401-405 MHz. The proposed antenna can
cover this frequency range if it is embedded in
an appropriate dielectric material. For this
purpose the antenna was embedded in
distilled water at 37°C with average
permittivity of
Measured and simulated return loss
Fig. 4. Measured and simulated return loss for the antenna in free space
with input impedance of 200 ohm.
The return loss and radiation patterns of the
fabricated antenna were measured. Figure 4
shows the simulated and measured return loss
versus frequency. As seen, the antenna has a
return loss of less than 8 dB for the entire
desired frequency band. The measurement
and simulation results are in close agreement.
Gain Vs Frequency
The maximal far-field antenna gain is depicted in Fig. 5.
As seen, the antenna gain varies within 4-7.5 dBi in the
frequency range. The antenna radiation pattern was
measured inside an anechoic chamber with far-field
facility.
Measured and simulated radiation
pattern for the E-plane and H-plane
(a)
Fig. 6. Measured and simulated radiation pattern of the spiral antenna for
the E-plane and H-plane at (a) 3 GHz, (b) 4 GHz, and (c) 5 GHz.
The measured and simulated radiation
patterns of the antenna for the E and H planes
for the frequencies of 3,4, and 5 GHz are
shown in Fig. 6. Due to the antenna’s directive
pattern one can expect high near-field
intensity in the broadside direction, which is
desirable for in-body usage.
Return loss versus frequency for
different material
The antenna was also simulated as if it were
embedded in different materials of
permittivity equal to 12, 27, and 50.The
corresponding port impedances varied within
40-60Ω. After matching the antenna, the
computed return loss was obtained and is
illustrated in Fig. 7. As seen, the operating
frequency range varies in each case, but all
the materials can provide good matching
within 750-1000 MHz.
Scenario of the spiral antenna near an
anatomical model
• This human model includes different bilogical
tissues. The simulation scenario of the
antenna close to the human body is illustrated
in Fig. 8.
Spectrum of the penetrating wave
• The average of the electric field intensity
versus frequency was computed and the
results are illustrated in Fig. 9 for each depth
plane for the antenna embedded in distilled
water. As seen, the field intensity diminishes
as frequency increases due to the larger
conductivity of the biological tissues at higher
frequencies.
Electric
field intensity inside the body versus depth
Figure 10 shows the average electric field
intensity for the x-axis component of the field.
As seen, the electric field intensity is highest
for the permittivity value of 27 in comparison
to the other permittivity values.
CONCLUSION
• A new design of an ultra-wideband spiral helical antenna
was presented for biomedical applications. In free space,
the antenna covers the frequency band of 3-10 GHz and
provides a directive pattern with high field intensity in its
aperture. If the antenna is embedded in distilled water
then it can operate in 300-1000 MHz. In proximity of the
human body, it was shown that a material with a
permittivity value of 27 serves well as a matching layer
providing the best wave penetration.
• Although this study was conducted for the chest, the same
procedure can be followed for the abdomen aimed at
applications like wireless capsule endoscope
communications.

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Antenna in body communication material

  • 2. Presentation On “An Ultra-Wideband Wire Spiral Antenna for In-Body Communications Using Different Material Matching Layers.”
  • 3. Author By • Ali Khaleghi • Ilangko Balasingham and • Raúl Chávez-Santiago
  • 4. Presented TO Md. Imran Khan Lecturer Dept. Of Electrical and Electronic Engineering World University Of Bangladesh
  • 5. Presented By Abdul Kader Id No: WUB 09/13/52/2102 & Md. Rabiul Alam Sourav Id No: WUB 09/13/52/2091
  • 6. Contents • Abstract • Introduction • Antenna Design • Measured and simulated return loss • Gain Vs Frequency • Measured and simulated radiation pattern for the E- plane and H-plane • Return loss versus frequency for different material • Scenario of the spiral antenna near an anatomical model
  • 7. Abstract 1. Used for getting information from human body. 2. Operating frequency 3-10 GHz and impedance 200 ohm in free space and permittivity values ranging from 12-74. 3. The best improvement in wave penetration was obtained for the frequency is 750-1000 MHz and inside material permittivity is 27.
  • 8. Introduction • This compact antenna is required for a number of diagnostic and therapeutic applications. • A properly designed antenna can transmit /receive to/from an implanted device over a significant part of the radio spectrum or transfer electromagnetic (EM) energy to internal organs. • The main problem in these applications is suffered in biological tissues.
  • 9. Introduction • The proposed antenna design has an impedance of 30-60 Ω . (according to material) • Example: When embedded in distilled water with permittivity equal to 74, the antenna covers the frequency range of 300- 1000 MHz.
  • 10. Ultra wide Band USES: UWB has several potential applications in medicine. Other uses are: Increasing data rate , a microwave hyperthermia applicator , microwave imaging radar etc.
  • 11. Antenna Design Fig. 1. Dual Spiral Archimedes antenna on top of a ground plane Fig. 2. Photography of the fabricated antenna and the matching unit.
  • 12. Fig. 3. Antenna impedance versus frequency in free space.
  • 13. Most wireless implantable medical devices operate in the narrowband frequency band of 401-405 MHz. The proposed antenna can cover this frequency range if it is embedded in an appropriate dielectric material. For this purpose the antenna was embedded in distilled water at 37°C with average permittivity of
  • 14. Measured and simulated return loss Fig. 4. Measured and simulated return loss for the antenna in free space with input impedance of 200 ohm.
  • 15. The return loss and radiation patterns of the fabricated antenna were measured. Figure 4 shows the simulated and measured return loss versus frequency. As seen, the antenna has a return loss of less than 8 dB for the entire desired frequency band. The measurement and simulation results are in close agreement.
  • 17. The maximal far-field antenna gain is depicted in Fig. 5. As seen, the antenna gain varies within 4-7.5 dBi in the frequency range. The antenna radiation pattern was measured inside an anechoic chamber with far-field facility.
  • 18. Measured and simulated radiation pattern for the E-plane and H-plane (a)
  • 19.
  • 20. Fig. 6. Measured and simulated radiation pattern of the spiral antenna for the E-plane and H-plane at (a) 3 GHz, (b) 4 GHz, and (c) 5 GHz.
  • 21. The measured and simulated radiation patterns of the antenna for the E and H planes for the frequencies of 3,4, and 5 GHz are shown in Fig. 6. Due to the antenna’s directive pattern one can expect high near-field intensity in the broadside direction, which is desirable for in-body usage.
  • 22. Return loss versus frequency for different material
  • 23. The antenna was also simulated as if it were embedded in different materials of permittivity equal to 12, 27, and 50.The corresponding port impedances varied within 40-60Ω. After matching the antenna, the computed return loss was obtained and is illustrated in Fig. 7. As seen, the operating frequency range varies in each case, but all the materials can provide good matching within 750-1000 MHz.
  • 24. Scenario of the spiral antenna near an anatomical model
  • 25. • This human model includes different bilogical tissues. The simulation scenario of the antenna close to the human body is illustrated in Fig. 8.
  • 26. Spectrum of the penetrating wave
  • 27. • The average of the electric field intensity versus frequency was computed and the results are illustrated in Fig. 9 for each depth plane for the antenna embedded in distilled water. As seen, the field intensity diminishes as frequency increases due to the larger conductivity of the biological tissues at higher frequencies.
  • 28. Electric field intensity inside the body versus depth
  • 29. Figure 10 shows the average electric field intensity for the x-axis component of the field. As seen, the electric field intensity is highest for the permittivity value of 27 in comparison to the other permittivity values.
  • 30. CONCLUSION • A new design of an ultra-wideband spiral helical antenna was presented for biomedical applications. In free space, the antenna covers the frequency band of 3-10 GHz and provides a directive pattern with high field intensity in its aperture. If the antenna is embedded in distilled water then it can operate in 300-1000 MHz. In proximity of the human body, it was shown that a material with a permittivity value of 27 serves well as a matching layer providing the best wave penetration. • Although this study was conducted for the chest, the same procedure can be followed for the abdomen aimed at applications like wireless capsule endoscope communications.