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Contact-based Radar Measurement of Cardiac Motion — A Position and Polarization Study Songjie Bi * , Juan Zeng * , Marzhan Bekbalanova * , Dennis Matthews # , and Xiaoguang “Leo” Liu * * University of California Davis, USA; # Cardiac Motion LLC., USA [email protected] Abstract— This paper presents quadrature demodulated data on cardiac motion from contact-based measurement using a Doppler radar and a planar antenna. Measurements were taken at several different locations on the chest of the test subject with both vertical and horizontal polarizations. Test data reveals different characteristics in terms of signal amplitude and time-domain waveform depending on the loca- tion/polarization, which shows the potential of using contact- based radar measurement for heart monitoring applications. Index Terms— radar, vital sign I. I NTRODUCTION There has been a surging interest in vital sign detection using Doppler radars in recent years [1]–[4]. The majority of the reported works, however, focus on remote detec- tion with the radar sensor placed at a distance from the subject under test. Due to the large difference in material properties (mainly the permittivity and conductivity) of the skin and the air, remote radar-based detection of vital signs relies on the measurement of the movement of the skin- air interface induced by the actual cardiac and respiration movements. Recently, we reported results from contact-based mea- surement of the cardiac motion with the radar antenna placed in contact with the skin [5]. The results revealed interesting characteristics in the radar return signals. Most notable is the fact that the return signals are dependent on where the antenna is attached to the chest, which implies that more information of the detailed heart movement may be obtained by contact-based measurement. However, our previous works relied a simple passive mixer to down- convert the received signal, which may lose significant information and lead to distortion of the radar return signal. In this work, we demonstrate position dependent contact-based measurement of cardiac motion using a quadrature radar receiver. We also demonstrate that such measurement is dependent on the antenna polarization. II. METHOD Fig. 1 shows the measurement setup used in this work. A Texas Instruments TRF371135 quadrature receiver in- tegrated circuit (IC) is used as a direct-conversion re- ceiver for demodulating the return signal. In addition to a quadrature mixer, the TRF371135 IC has built-in baseband amplification and dc-offset calibration. The transmitted signal is generated by a Hittite HMC385 voltage controlled oscillator (VCO) and amplified by a Hittite HMC374 power amplifier. The components are integrated on a custom-designed printed circuit board (PCB) with edge- mount connectors for the antennas. In our experiment, 2.4 GHz is arbitrarily chosen to be the operating frequency. I-Channel Q- Channel Power ECG Amp SPI 1 2 3 4 ECG Lead ECG Lead π/2 I Q (a) (b) (c) Fig. 1. (a) General schematic of the radar system. (b) Picture of the measurement setup. (c) Four measurement locations. A simple planar dipole antenna fabricated on an FR- 4 substrate is used in the measurement. The center con- ductor and the ground shield of the antenna feed-line are connected to the two arms of the dipole through an SMB connector. The antenna is designed to operate in contact with the chest. Realistic material properties of human tissues are used in the design to ensure good impedance matching [6]. In a contact-based measurement, it is necessary to use a single antenna for both transmit (TX) and receive (RX) if

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Page 1: Contact-based Radar Measurement of Cardiac Motion — A ...dart.ece.ucdavis.edu/publication/sjbi2016.pdfdemodulation is used to extract the object movement. An implicit assumption

Contact-based Radar Measurement of Cardiac Motion — APosition and Polarization Study

Songjie Bi ∗, Juan Zeng ∗, Marzhan Bekbalanova ∗, Dennis Matthews #, and Xiaoguang “Leo” Liu ∗

∗University of California Davis, USA; # Cardiac Motion LLC., [email protected]

Abstract— This paper presents quadrature demodulateddata on cardiac motion from contact-based measurementusing a Doppler radar and a planar antenna. Measurementswere taken at several different locations on the chest of thetest subject with both vertical and horizontal polarizations.Test data reveals different characteristics in terms of signalamplitude and time-domain waveform depending on the loca-tion/polarization, which shows the potential of using contact-based radar measurement for heart monitoring applications.

Index Terms— radar, vital sign

I. INTRODUCTION

There has been a surging interest in vital sign detectionusing Doppler radars in recent years [1]–[4]. The majorityof the reported works, however, focus on remote detec-tion with the radar sensor placed at a distance from thesubject under test. Due to the large difference in materialproperties (mainly the permittivity and conductivity) of theskin and the air, remote radar-based detection of vital signsrelies on the measurement of the movement of the skin-air interface induced by the actual cardiac and respirationmovements.

Recently, we reported results from contact-based mea-surement of the cardiac motion with the radar antennaplaced in contact with the skin [5]. The results revealedinteresting characteristics in the radar return signals. Mostnotable is the fact that the return signals are dependent onwhere the antenna is attached to the chest, which impliesthat more information of the detailed heart movement maybe obtained by contact-based measurement. However, ourprevious works relied a simple passive mixer to down-convert the received signal, which may lose significantinformation and lead to distortion of the radar return signal.

In this work, we demonstrate position dependentcontact-based measurement of cardiac motion using aquadrature radar receiver. We also demonstrate that suchmeasurement is dependent on the antenna polarization.

II. METHOD

Fig. 1 shows the measurement setup used in this work.A Texas Instruments TRF371135 quadrature receiver in-tegrated circuit (IC) is used as a direct-conversion re-ceiver for demodulating the return signal. In addition to a

quadrature mixer, the TRF371135 IC has built-in basebandamplification and dc-offset calibration. The transmittedsignal is generated by a Hittite HMC385 voltage controlledoscillator (VCO) and amplified by a Hittite HMC374power amplifier. The components are integrated on acustom-designed printed circuit board (PCB) with edge-mount connectors for the antennas. In our experiment,2.4 GHz is arbitrarily chosen to be the operating frequency.

I-Channel

Q-Channel

Power

ECGAmp

SPI

1

23 4

ECGLead

ECGLead

π/2I

Q

(a)

(b) (c)

Fig. 1. (a) General schematic of the radar system. (b) Pictureof the measurement setup. (c) Four measurement locations.

A simple planar dipole antenna fabricated on an FR-4 substrate is used in the measurement. The center con-ductor and the ground shield of the antenna feed-line areconnected to the two arms of the dipole through an SMBconnector. The antenna is designed to operate in contactwith the chest. Realistic material properties of humantissues are used in the design to ensure good impedancematching [6].

In a contact-based measurement, it is necessary to use asingle antenna for both transmit (TX) and receive (RX) if

Page 2: Contact-based Radar Measurement of Cardiac Motion — A ...dart.ece.ucdavis.edu/publication/sjbi2016.pdfdemodulation is used to extract the object movement. An implicit assumption

monostatic detection is desired. This is due to the relativelyshort distance between the antenna and the heart. Becauseof the finite size of the antenna, using two of them side byside will result in effectively a bi-static measurement andthe close distance between the two antennas may lead tointerference and dc-offset issues. Therefore, a circulator isused so that TX and RX can share the same antenna.

In the tests, the antenna is placed firmly against thetest subject’s chest1 to eliminate the effect of the skinmovement. To eliminate the movement due to respiration,the test subject holds his breath during the measurement.Measurements are taken with the antenna placed at fourdifferent locations, labeled 1-4 in Fig. 1-c. At each loca-tion, measurements with both horizontal and vertical an-tenna polarization are taken. In addition, electrocardiogram(ECG) measurement is also taken simultaneously with theradar measurement, providing time-correlation between thetwo.

III. MEASUREMENT RESULTS AND DISCUSSION

Fig. 2 presents the measurement data, including the in-phase and quadrature data as well as the time-correlatedECG data, at the four measurement locations with bothvertical and horizontal antenna polarization.

Although the test subject held the breath during themeasurement, a slow drift of the measured signal can stillbe observed. The baseline of this slow drift can be fittedfrom the peaks—or any other distinguishing feature of thesignal within a cardiac cycle—from the measurement data.The measured I/Q data can then be corrected by subtractingthe fitted baseline drift. In order not to corrupt the relativemagnitude of the I/Q data, the first cardiac cycle from eachmeasurement is used as a reference. In Fig. 2-f, we haveincluded an example where both the raw measurement dataand the corrected one are presented.

Radar measurement data shows at different measure-ment locations and polarizations. For example, measure-ment at location 3, which is on the right side of the body,is much weaker in magnitude2. This may be due to thefact that the antenna is farther away from the heart thanthe other locations. Variations due to polarization may beattributed to the complex geometry and motion of the heart.

In the current literature, arctangent or complex signaldemodulation is used to extract the object movement. Animplicit assumption made is that the object is located inthe far field where the phase change of the return signalis linearly proportional to the distance between the radarand the object. In a contact-based measurement of cardiacmotion, it is likely that this assumption can no longer beheld true. The short distance between the antenna and theheart muscle means that the cardiac movement is in thenear-field region of the antenna. Further theoretical and

1The test subject is a 33 year old male with average weigth.2Worth pointing out is that the vertical scale for the plots are different.

experimental studies are needed to understand the exactdistance-phase difference.

In remote radar measurement, the return signal am-plitude variation can be neglected because of the smallmovement (0.1–1 mm) relative to the stand-off distance(>1 m). On the complex I/Q plane, the return signaltrajectory follows an arc. In contact-based measurement,however, amplitude variation can no longer be neglecteddue to the relative close distance between the antenna andthe heart. This effect manifests itself as an excursion alongthe radial direction on the complex I/Q plane (Fig. 3).

Q-Channel (V)0 0.2 0.4 0.6 0.8

I-Cha

nnel

(V)

-1.4

-1.2

-1

-0.8

-0.6

(0.42, -1.02)

0.33

5

Fig. 3. I vs. Q plot of measurement (g).

IV. CONCLUSION

We have presented measurement data related to phys-iological movement inside the thorax cavity, particularlycardiac movement, based on contact-based radar measure-ment. Compared with previous work using remote mea-surement, the presented data shows significant variationin time-domain waveforms depending on the location andpolarization of the antenna. Such data may shed light onthe detailed movement profile of the heart and may beuseful for health monitoring applications.

REFERENCES

[1] C. Li, J. Cummings, J. Lam, E. Graves, and W. Wu, “Radar remotemonitoring of vital signs,” IEEE Microwave Magazine, vol. 10, pp.47–56, 2009.

[2] C. Li, X. Yu, C.-M. Lee, D. Li, L. Ran, and J. Lin, “High-sensitivitysoftware-configurable 5.8-ghz radar sensor receiver chip in 0.13-µmcmos for noncontact vital sign detection,” IEEE Transactions onMicrowave Theory and Techniques, vol. 58, pp. 1410–1419, 2010.

[3] F.-K. Wang, T.-S. Horng, K.-C. Peng, J.-K. Jau, J.-Y. Li, and C.-C.Chen, “Single-antenna doppler radars using self and mutual injectionlocking for vital sign detection with random body movement can-cellation,” IEEE Transactions on Microwave Theory and Techniques,vol. 59, no. 12, pp. 3577–3587, Dec. 2011.

[4] J. Lin and W. Wu, “Vital sign radars: Past, present, and future,”in 2014 IEEE 15th Annual Wireless and Microwave TechnologyConference (WAMICON), 2014.

[5] S. Bi, X. Liu, and D. Matthews, “An experimental study of 2-dcardiac motion pattern based on contact radar measurement,” in 2015IEEE 16th Annual Wireless and Microwave Technology Conference(WAMICON), 2015.

[6] J. W. Penn and E. L. Bell, “Electrical parameter values of somehuman tissues in the radio frequency radiation range,” USAF Schoolof Medicine, Tech. Rep., 1978.

Page 3: Contact-based Radar Measurement of Cardiac Motion — A ...dart.ece.ucdavis.edu/publication/sjbi2016.pdfdemodulation is used to extract the object movement. An implicit assumption

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0 1 2 3 4 5−0.78−0.73−0.68

0 1 2 3 4 50.080.130.18

(h)

0 1 2 3 4 51.551.601.65

0 1 2 3 4 5−0.240−0.215−0.190

0 1 2 3 4 5−1.080−1.055−1.030

(f)(e)

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0 1 2 3 4 5−1.40−1.35−1.30

3. R

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0 1 2 3 4 50.60.70.8

(d)

0 1 2 3 4 51.551.601.65

0 1 2 3 4 5−1.15−1.05−0.95

0 1 2 3 4 50.30.40.5

(a)

0 1 2 3 4 51.551.601.65

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Vertical Polarization Horizontal Polarization

EC

G (V

)I (

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(V)

Time (s)

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(V)

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Time (s)

Fig. 2. Contact-based radar measurement of cardiac motion. (a-d) represent measurement taken from location 1-4, each with time-correlated ECG measurement.