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Journal for Research| Volume 01| Issue 07 | September 2015
ISSN: 2395-7549
All rights reserved by www.journalforresearch.org 1
Novel Methodology of the Ultra Sonic Beam in
Linear Array Transducer for High Frequency
Applications
N.S Murti Sarma Oruganti Madhu
Department of Electronics & Communications Engineering Department of Electronics & Communications Engineering
Sreenidhi Institute of Science and Technology, Yamnampet,
Ghatakesar-501301
Sreenidhi Institute of Science and Technology, Yamnampet,
Ghatakesar-501301
S.P.Venu Madhava Rao
Department of Electronics & Communications Engineering
Sreenidhi Institute of Science and Technology, Yamnampet, Ghatakesar-501301
Abstract
In this paper, the focusing of ultrasound beam is considered. Electronic circuitry is considered as support to the theme of the
work. The results presented in this paper are notable for improved resolution. The extension of the application diversity is also
proposed based on use of Piezo electric transceducers.
Keywords: Ultrasonic, Linear Array, Real Time Image, Beam Divergence, Piezo-Electrictransceducers
_______________________________________________________________________________________________________
I. INTRODUCTION
Arrays are in general popular for better directive properties of radiating elements. These are well known for ease of extendibility
of concept[1]. Linear array transducer is the most important and sophisticate component of the transducer used in medical
imaging that produces the ultrasonic beam [2-10]. The proposal may also through light to power harvesting in cases such as
Street lights and mobile phones[11-15]. This beam is focused to the origin under scanning and a real time image of that particular
organ is seen on the vedio monitor in B mode. Typical linear array transducer consists of a long strip of piezo electric ceramic
divided into a number of closely spaced rectangular elements arranged side by side along with damping material, RF shield,
matching layer, focusing lens and switching electronic circuits[2].
In this paper, the application of antenna arrays is conceptualized for ultrasonic arrays is a new attempt in this paper.
This paper is organized into 4 sections. Except the sec.2, the rest of the sections are conventional.
Fig. 1: Near & Far field of Ultra Sonic Beam with Array of Element
II. OUTLINE OF THE WORK
The rectangular configuration (Fig.1) of array transducer element causes an ultrasound beam to be generated. The individual
element radiation expressed mathematically as
F(θ)=λsin(π/asinθ)/(π/asinθ) (1)
Where F is field amplitude, a is element width , λ is wave length (m)and
θ=sin{1.22(λ/D)} (2)
is measurement angle in degrees[2]. From (1) and (2), states that the ultra sonic amplitude at an angle θ is related to element
width and wavelength. The terminology designated the wavelength with meter as unit in general convention. However, based on
the frequency the unit will be in the order of even mm also. These two variable contribute equally to the ultrasonic field
Novel Methodology of the Ultra Sonic Beam in Linear Array Transducer for High Frequency Applications
(J4R/ Volume 01 / Issue 07 / 001)
All rights reserved by www.journalforresearch.org 2
characteristics of a single rectangular element.(See Fig.1). It can be seen from the equation that increasing both element width
and frequency produces more directional beam from an individual element. If the individual elements of the array are pulsed
because of their small size results in a low sensitivity and poor lateral resolution due to beam divergence [2]. To overcome this
problem, the array elements are to be pulsed in multiple element groups.
Table – 1
Divison of Array Elements In Groups
S.No Element numbers
1 1 9 17 25 33 41 49 57
2 2 10 18 26 34 42 50 58
3 3 11 19 27 35 43 51 59
4. 4 12 20 28 36 44 52 60
5. 5 13 21 29 37 45 53 61
6 6 14 22 30 38 46 54 62
7 7 15 23 31 39 47 55 63
8. 8 16 24 32 40 48 56 64
Electronic FocusingA.
Normally each element has to have its own transmitter and its own receiver. This transmitter and receiver have to be switched on
and off by command. However, to reduce the number of transmitters and receivers, the elements are organized into groups. Each
group has one transmitter and one receiver which can be multiplexed to the appropriate elements. Here an array of 64 elements is
taken and grouped into eight groups for better results (See Table 1). In this table First column of the table should be understand
as group number.
III.RESULTS AND DISCUSSION
The elements in groups are excited to receive the echoes from the array elements the certain time delay (See Fig.2,3). Each array
element that is activated produces a wavefront.
Fig.2: Eight element array
All these wave fronts together interfering in to one large resultant wave front. The focused wave front is achieved by
activating the elements with small time differences. These are properly compensated by means of delay lines[3]. The transmitter
and receiver delay settings are the factors that influence the lateral resolution. For this the target must lie within the near field
zone of the group of the elements. This is achieved with the help of beam focusing.
Fig. 3: Acoustic Array
The beam focused by activating 64 elements, the group of 8 elements each provides improved lateral and axial resolution of
the target The electronic focusing of the ultrasonic beam is done in dividing the individual elements in to groups. The individual
Novel Methodology of the Ultra Sonic Beam in Linear Array Transducer for High Frequency Applications
(J4R/ Volume 01 / Issue 07 / 001)
All rights reserved by www.journalforresearch.org 3
elements are excited in groups. Each element in group is activated electronically, delayed and resultant wave front that is
electronically focused provides better resolution of the images (Fig.4 and 5). This beam is focused to the origin under scanning
and a real time image of that particular organ is seen on the vedio monitor in B mode[4].
Fig. 4: Beam with Focusing
Fig. 5: Beam with Focusing
IV.CONCLUSIONS
In this paper, the application of antenna arrays is conceptualized for ultrasonic arrays is a new attempt in this paper. A linear
array is considered in our attempt. The tranceducer concept in this paper is by using electronic circuitry. The transmitter and
receiver delay settings are the factors that influence the lateral resolution. Its found vast applications in medical imaging field on
extension of array concept for transceducers. The application is not restricted to medical field. The same can be proposed to
power harvesting in cases of Street lights and mobile phones. However, the proposal of power harvesting case, wireless
communication principle is used. At the first of the exercise, these two cases planed using piezo electric transceducers. On
sucessfullness of the attempt at microscale, the concept will be raised to support the power requirements domestic purposes also.
ACKNOWLEDGEMENTS
Prior to compilation of this paper, the authors proposed a minor research proposal based on transeducer application. It is under
consideration of UGC with file number ROMRP-SERO-ELEC-2015-16-65651 , 13,August2015. Authors are thankful for
initiation of such schemes. Acknowledgements are also due for Dr. Poreddy Narasimha Reddy, Director of SNIST for his
interest in the work. S.Sambaih of Vasavi Engeering college ibrahimpatnam deserves due acknowledgements for his support in
our work.
REFERENCES
[1] Kraus, J.D, Marhefka and A. Ahmed Khan, “Antennas and Wave propagation”, 4e/TMH,2010.
[2] Taziev, R.M. "Surface and quasi-longitudinal acoustic waves in KTiOAsO4 and KTiOPO4 single crystals", Control and Communications (SIBCON),
International Siberian Conference , page(s): 1 – 4, 2013.
[3] Sambiah,S, N.S.Murthy Sharma and K.V.S.V.R.Prasad, “A New Electronic Focussing Technique Of The Ultra Sonic Beam In Linear Array Tranceducer”,
Proc.RACE05, June, 2005.
[4] D. H. Turnbull and F .S. Foster, “Fabrication and characterstics of transducer elements in 2-D arrays for medical ultra sound”, IEEE Trans , Vol.38, July,
1992.
[5] Makukha, V.K.; Atuchin, Viktor V.; Kesler, V.G. "Core level spectroscopy of RbTiOPO4 and chemical bonding in KTiOPO4 crystal family",
Fundamental Problems of Micro/Nanosystems Technologies (MNST), IEEE 2nd Russia School and Seminar on, page(s): 7 – 10, 2010.
[6] D.K.T. Chue, J.D.Bielin, “ Piezo electric and acoustic properties of potassium titanine phosphate(KTP) and its isomorphs” IEEE, Trans Vol.39, Nov.,
1992.
Novel Methodology of the Ultra Sonic Beam in Linear Array Transducer for High Frequency Applications
(J4R/ Volume 01 / Issue 07 / 001)
All rights reserved by www.journalforresearch.org 4
[7] Turnbull D.H., and F.S.Foster, “Beam stearing with pulsed two dimensional transducer arrays”, Proceedings of IEEE, Vol.38, (Electronic version).
August,2002.
[8] James E. Moore Jr, Duncan J. Maitland, “ Biomedical technology and devices”CRC press,2013.
[9] Wells, PNT, “Biomedical ultrasonics”, Acadamic press, London, 1977.
[10] Matte GM, Van Neer PL, Danilouchkine MG, Huijssen J, Verweij MD, de Jong N., “Optimization of a phased-array transducer for multiple harmonic
imaging in medical applications: frequency and topology”, IEEE Trans Ultrason Ferroelectr Freq Control.VOl. 58 No.3:533-46. Mar2011.
[11] Mina, I.G, “High Frequency Transducers from PZT Films”, M.S Thesis, The Pennsylvania State University, May 2007.
[12] E. K. Reilly, L. M. Miller, R. Fain, and P. Wright, “A study of ambient vibrations for piezoelectric energy conversion,”Proc. PowerMEMS, pp. 312–315,
2009
[13] P. D. Mitcheson, E. M. Yeatman, G. K. Rao, A. S. Holmes, and T. C. Green, “Human and machine motion for wireless electronic devices,”Proc. IEEE, vol.
96, no. 9, pp. 1457–1486, Sep. 2008.
[14] M. Ferrari, V. Ferrari, D. Marioli, and A. Taroni, “Modeling, fabricationand performance measurements of a piezoelectric energy converter forpower
harvesting in autonomous icrosystems,”IEEETrans. Instrum.Meas., vol. 55, no. 6, pp. 2096–2101, Dec. 2006.
[15] S. Roundy and P. K. Wright, “A piezoelectric vibration based generator for wireless electronics,”Smart Mater. Struct., vol. 13, no. 5, pp. 1131–1142, Oct.
2004.

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NOVEL METHODOLOGY OF THE ULTRA SONIC BEAM IN LINEAR ARRAY TRANSDUCER FOR HIGH FREQUENCY APPLICATIONS

  • 1. Journal for Research| Volume 01| Issue 07 | September 2015 ISSN: 2395-7549 All rights reserved by www.journalforresearch.org 1 Novel Methodology of the Ultra Sonic Beam in Linear Array Transducer for High Frequency Applications N.S Murti Sarma Oruganti Madhu Department of Electronics & Communications Engineering Department of Electronics & Communications Engineering Sreenidhi Institute of Science and Technology, Yamnampet, Ghatakesar-501301 Sreenidhi Institute of Science and Technology, Yamnampet, Ghatakesar-501301 S.P.Venu Madhava Rao Department of Electronics & Communications Engineering Sreenidhi Institute of Science and Technology, Yamnampet, Ghatakesar-501301 Abstract In this paper, the focusing of ultrasound beam is considered. Electronic circuitry is considered as support to the theme of the work. The results presented in this paper are notable for improved resolution. The extension of the application diversity is also proposed based on use of Piezo electric transceducers. Keywords: Ultrasonic, Linear Array, Real Time Image, Beam Divergence, Piezo-Electrictransceducers _______________________________________________________________________________________________________ I. INTRODUCTION Arrays are in general popular for better directive properties of radiating elements. These are well known for ease of extendibility of concept[1]. Linear array transducer is the most important and sophisticate component of the transducer used in medical imaging that produces the ultrasonic beam [2-10]. The proposal may also through light to power harvesting in cases such as Street lights and mobile phones[11-15]. This beam is focused to the origin under scanning and a real time image of that particular organ is seen on the vedio monitor in B mode. Typical linear array transducer consists of a long strip of piezo electric ceramic divided into a number of closely spaced rectangular elements arranged side by side along with damping material, RF shield, matching layer, focusing lens and switching electronic circuits[2]. In this paper, the application of antenna arrays is conceptualized for ultrasonic arrays is a new attempt in this paper. This paper is organized into 4 sections. Except the sec.2, the rest of the sections are conventional. Fig. 1: Near & Far field of Ultra Sonic Beam with Array of Element II. OUTLINE OF THE WORK The rectangular configuration (Fig.1) of array transducer element causes an ultrasound beam to be generated. The individual element radiation expressed mathematically as F(θ)=λsin(π/asinθ)/(π/asinθ) (1) Where F is field amplitude, a is element width , λ is wave length (m)and θ=sin{1.22(λ/D)} (2) is measurement angle in degrees[2]. From (1) and (2), states that the ultra sonic amplitude at an angle θ is related to element width and wavelength. The terminology designated the wavelength with meter as unit in general convention. However, based on the frequency the unit will be in the order of even mm also. These two variable contribute equally to the ultrasonic field
  • 2. Novel Methodology of the Ultra Sonic Beam in Linear Array Transducer for High Frequency Applications (J4R/ Volume 01 / Issue 07 / 001) All rights reserved by www.journalforresearch.org 2 characteristics of a single rectangular element.(See Fig.1). It can be seen from the equation that increasing both element width and frequency produces more directional beam from an individual element. If the individual elements of the array are pulsed because of their small size results in a low sensitivity and poor lateral resolution due to beam divergence [2]. To overcome this problem, the array elements are to be pulsed in multiple element groups. Table – 1 Divison of Array Elements In Groups S.No Element numbers 1 1 9 17 25 33 41 49 57 2 2 10 18 26 34 42 50 58 3 3 11 19 27 35 43 51 59 4. 4 12 20 28 36 44 52 60 5. 5 13 21 29 37 45 53 61 6 6 14 22 30 38 46 54 62 7 7 15 23 31 39 47 55 63 8. 8 16 24 32 40 48 56 64 Electronic FocusingA. Normally each element has to have its own transmitter and its own receiver. This transmitter and receiver have to be switched on and off by command. However, to reduce the number of transmitters and receivers, the elements are organized into groups. Each group has one transmitter and one receiver which can be multiplexed to the appropriate elements. Here an array of 64 elements is taken and grouped into eight groups for better results (See Table 1). In this table First column of the table should be understand as group number. III.RESULTS AND DISCUSSION The elements in groups are excited to receive the echoes from the array elements the certain time delay (See Fig.2,3). Each array element that is activated produces a wavefront. Fig.2: Eight element array All these wave fronts together interfering in to one large resultant wave front. The focused wave front is achieved by activating the elements with small time differences. These are properly compensated by means of delay lines[3]. The transmitter and receiver delay settings are the factors that influence the lateral resolution. For this the target must lie within the near field zone of the group of the elements. This is achieved with the help of beam focusing. Fig. 3: Acoustic Array The beam focused by activating 64 elements, the group of 8 elements each provides improved lateral and axial resolution of the target The electronic focusing of the ultrasonic beam is done in dividing the individual elements in to groups. The individual
  • 3. Novel Methodology of the Ultra Sonic Beam in Linear Array Transducer for High Frequency Applications (J4R/ Volume 01 / Issue 07 / 001) All rights reserved by www.journalforresearch.org 3 elements are excited in groups. Each element in group is activated electronically, delayed and resultant wave front that is electronically focused provides better resolution of the images (Fig.4 and 5). This beam is focused to the origin under scanning and a real time image of that particular organ is seen on the vedio monitor in B mode[4]. Fig. 4: Beam with Focusing Fig. 5: Beam with Focusing IV.CONCLUSIONS In this paper, the application of antenna arrays is conceptualized for ultrasonic arrays is a new attempt in this paper. A linear array is considered in our attempt. The tranceducer concept in this paper is by using electronic circuitry. The transmitter and receiver delay settings are the factors that influence the lateral resolution. Its found vast applications in medical imaging field on extension of array concept for transceducers. The application is not restricted to medical field. The same can be proposed to power harvesting in cases of Street lights and mobile phones. However, the proposal of power harvesting case, wireless communication principle is used. At the first of the exercise, these two cases planed using piezo electric transceducers. On sucessfullness of the attempt at microscale, the concept will be raised to support the power requirements domestic purposes also. ACKNOWLEDGEMENTS Prior to compilation of this paper, the authors proposed a minor research proposal based on transeducer application. It is under consideration of UGC with file number ROMRP-SERO-ELEC-2015-16-65651 , 13,August2015. Authors are thankful for initiation of such schemes. Acknowledgements are also due for Dr. Poreddy Narasimha Reddy, Director of SNIST for his interest in the work. S.Sambaih of Vasavi Engeering college ibrahimpatnam deserves due acknowledgements for his support in our work. REFERENCES [1] Kraus, J.D, Marhefka and A. Ahmed Khan, “Antennas and Wave propagation”, 4e/TMH,2010. [2] Taziev, R.M. "Surface and quasi-longitudinal acoustic waves in KTiOAsO4 and KTiOPO4 single crystals", Control and Communications (SIBCON), International Siberian Conference , page(s): 1 – 4, 2013. [3] Sambiah,S, N.S.Murthy Sharma and K.V.S.V.R.Prasad, “A New Electronic Focussing Technique Of The Ultra Sonic Beam In Linear Array Tranceducer”, Proc.RACE05, June, 2005. [4] D. H. Turnbull and F .S. Foster, “Fabrication and characterstics of transducer elements in 2-D arrays for medical ultra sound”, IEEE Trans , Vol.38, July, 1992. [5] Makukha, V.K.; Atuchin, Viktor V.; Kesler, V.G. "Core level spectroscopy of RbTiOPO4 and chemical bonding in KTiOPO4 crystal family", Fundamental Problems of Micro/Nanosystems Technologies (MNST), IEEE 2nd Russia School and Seminar on, page(s): 7 – 10, 2010. [6] D.K.T. Chue, J.D.Bielin, “ Piezo electric and acoustic properties of potassium titanine phosphate(KTP) and its isomorphs” IEEE, Trans Vol.39, Nov., 1992.
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