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Journal articles on the topic 'Doppler effect'

Author: Grafiati
Published: 4 June 2021
Last updated: 30 July 2024

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1

Ballard, Megan S. "Doppler effect." Journal of the Acoustical Society of America 127, no. 3 (March 2010): 1912. http://dx.doi.org/10.1121/1.3384841.

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2

Klinaku, Shukri. "Time Doppler effect." Physics Essays 29, no. 1 (March 10, 2016): 113–16. http://dx.doi.org/10.4006/0836-1398-29.1.113.

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3

WATANABE, Kazumi. "Elastodynamic Doppler Effect." Proceedings of the 1992 Annual Meeting of JSME/MMD 2003 (2003): 553–54. http://dx.doi.org/10.1299/jsmezairiki.2003.0_553.

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4

Morehouse, Roger. "Doppler-effect equations." Physics Teacher 35, no. 8 (November 1997): 509–11. http://dx.doi.org/10.1119/1.2344783.

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5

Hanna, R. C. "Acoustic Doppler effect." Physics Education 23, no. 1 (January 1, 1988): 8. http://dx.doi.org/10.1088/0031-9120/23/1/102.

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6

Kantor, Wallace. "Doppler Effect Reconsidered." Fortschritte der Physik/Progress of Physics 40, no. 1 (1992): 73–91. http://dx.doi.org/10.1002/prop.2190400104.

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7

Eska, Andrita Ceriana. "Doppler Shift Effect at The Communication Systems with 10 GHz around Building." JURNAL INFOTEL 12, no. 4 (November 25, 2020): 129–33. http://dx.doi.org/10.20895/infotel.v12i4.483.

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This research described the Doppler shift effect for the communication systems. The mobile station moves with various velocities around the building’s environment. Doppler’s shift influences the communication systems. The frequency communication was used 10 GHz and its influenced by atmospheric attenuation. This research consisted of propagation with LOS and NLOS conditions, mobile station velocity variation, height buildings variation, and transmitter power variation. This research described frequency maximum at Doppler shift, coherence time, and signal to noise ratio. More increase Doppler shift of coherence time caused signal noise ratio to decrease.
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8

Lee, Chang-Young. "Analysis of Formula 1 Sound by Doppler Effect." JOURNAL OF THE ACOUSTICAL SOCIETY OF KOREA 32, no. 5 (2013): 385. http://dx.doi.org/10.7776/ask.2013.32.5.385.

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9

Ryazantsev, O. V., S. V. Мarchenko, and M. V. Kulik. "On the Doppler effect in radar." Radiotekhnika, no. 204 (April 9, 2021): 93–98. http://dx.doi.org/10.30837/rt.2021.1.204.10.

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The possibilities of simultaneous use of the longitudinal and transverse Doppler effects have been analyzed, and expressions have been derived for the corresponding beat frequencies between the emitted and received signals. As a rule, only the longitudinal Doppler effect is used in modern radio engineering systems, which makes it possible to determine the radial component of the object's speed. In addition, there are situations for which it is generally impossible to determine the speed of an object without taking into account the transverse Doppler effect. The authors analyze the fundamental possibilities of improving the functioning of radar stations that simultaneously use both types of Doppler effects – longitudinal and transverse ones – making it possible to determine the total speed of the observed object in any situations. The authors have analyzed the longitudinal and transverse Doppler effects for the case of a moving emitting object, derived expressions for the Doppler shift and expressions for the beat frequency in the case of an active radar station for both types of Doppler effects, which make it possible to obtain the value of the object's speed in any situations. Variants of determining the total speed of a moving object have been proposed, accounting the determination of its radial and tangential components. Idealized situations in which only one of the Doppler effects appeared have been considered.
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10

Klinaku, Shukri. "New Doppler effect formula." Physics Essays 29, no. 4 (December 5, 2016): 506–7. http://dx.doi.org/10.4006/0836-1398-29.4.506.

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11

Shi, Xihang, Xiao Lin, Ido Kaminer, Fei Gao, Zhaoju Yang, John D. Joannopoulos, Marin Soljačić, and Baile Zhang. "Superlight inverse Doppler effect." Nature Physics 14, no. 10 (July 9, 2018): 1001–5. http://dx.doi.org/10.1038/s41567-018-0209-6.

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12

Marrucci, L. "Spinning the Doppler Effect." Science 341, no. 6145 (August 1, 2013): 464–65. http://dx.doi.org/10.1126/science.1242097.

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13

Deng, Junhong, King Fai Li, Wei Liu, and Guixin Li. "Cascaded rotational Doppler effect." Optics Letters 44, no. 9 (April 29, 2019): 2346. http://dx.doi.org/10.1364/ol.44.002346.

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14

Bachman, R. A. "Generalized relativistic Doppler effect." American Journal of Physics 54, no. 8 (August 1986): 717–19. http://dx.doi.org/10.1119/1.14479.

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15

Varnier, Jean. "Doppler effect in aeroacoustics." Journal of the Acoustical Society of America 123, no. 5 (May 2008): 3248. http://dx.doi.org/10.1121/1.2933517.

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16

Brasselet, Etienne. "Harmonic angular Doppler effect." Nature Photonics 10, no. 6 (May 31, 2016): 362–64. http://dx.doi.org/10.1038/nphoton.2016.106.

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17

Caruso, Eugene M., Leaf Van Boven, Mark Chin, and Andrew Ward. "The Temporal Doppler Effect." Psychological Science 24, no. 4 (March 8, 2013): 530–36. http://dx.doi.org/10.1177/0956797612458804.

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18

Maughan, C., and G. Chadha. "The acoustic Doppler effect." Physics Education 22, no. 4 (July 1, 1987): 256–58. http://dx.doi.org/10.1088/0031-9120/22/4/313.

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19

Scharf, Rainer. "Optical Doppler effect inverted." Optik & Photonik 6, no. 2 (May 2011): 20. http://dx.doi.org/10.1002/opph.201190318.

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20

Luo, Ying, Yi‐Jun Chen, Yong‐Zhong Zhu, Wang‐Yang Li, and Qun Zhang. "Doppler effect and micro‐Doppler effect of vortex‐electromagnetic‐wave‐based radar." IET Radar, Sonar & Navigation 14, no. 1 (January 2020): 2–9. http://dx.doi.org/10.1049/iet-rsn.2019.0124.

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21

Gong, Jiangkun, Jun Yan, Deren Li, and Deyong Kong. "Detection of Micro-Doppler Signals of Drones Using Radar Systems with Different Radar Dwell Times." Drones 6, no. 9 (September 19, 2022): 262. http://dx.doi.org/10.3390/drones6090262.

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Not any radar dwell time of a drone radar is suitable for detecting micro-Doppler (or jet engine modulation, JEM) produced by the rotating blades in radar signals of drones. Theoretically, any X-band drone radar system should detect micro-Doppler of blades because of the micro-Doppler effect and partial resonance effect. Yet, we analyzed radar data detected by three radar systems with different radar dwell times but similar frequency and velocity resolution, including Radar−α, Radar−β, and Radar−γ with radar dwell times of 2.7 ms, 20 ms, and 89 ms, respectively. The results indicate that Radar−β is the best radar for detecting micro-Doppler (i.e., JEM signals) produced by the rotating blades of a quadrotor drone, DJI Phantom 4, because the detection probability of JEM signals is almost 100%, with approximately 2 peaks, whose magnitudes are similar to that of the body Doppler. In contrast, Radar−α can barely detect any micro-Doppler, and Radar−γ detects weak micro-Doppler signals, whose magnitude is only 10% of the body Doppler’s. Proper radar dwell time is the key to micro-Doppler detection. This research provides an idea for designing a cognitive micro-Doppler radar by changing radar dwell time for detecting and tracking micro-Doppler signals of drones.
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22

Sorokin, Yu M. "Doppler effect and aberrational effects in dispersive medium." Radiophysics and Quantum Electronics 36, no. 7 (July 1993): 410–22. http://dx.doi.org/10.1007/bf01040255.

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23

Sha, Qimeng, Song Qiu, Tong Liu, Weijie Wang, and Yuan Ren. "Doppler effect of polarization grating." Applied Optics 60, no. 10 (March 22, 2021): 2788. http://dx.doi.org/10.1364/ao.419013.

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24

Purnell, B. A. "Observing an embryonic Doppler effect." Science 345, no. 6193 (July 10, 2014): 175–77. http://dx.doi.org/10.1126/science.345.6193.175-p.

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25

Menon, V. J., and D. C. Agrawal. "Relativistic acoustic Doppler effect revisited." American Journal of Physics 53, no. 5 (May 1985): 483–84. http://dx.doi.org/10.1119/1.14205.

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26

Liang, N. K. "The typhoon swell Doppler effect." Ocean Engineering 30, no. 9 (June 2003): 1107–15. http://dx.doi.org/10.1016/s0029-8018(02)00099-9.

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27

Lambourne, Robert. "The Doppler effect in astronomy." Physics Education 32, no. 1 (January 1997): 34–40. http://dx.doi.org/10.1088/0031-9120/32/1/017.

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28

Vityaz, O. A. "Doppler effect and absolute motion." Electronics and Communications 16, no. 1 (March 28, 2011): 71–81. http://dx.doi.org/10.20535/2312-1807.2011.16.1.273945.

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Evidence of insolvency of the relativity theory postulate on the equality of inertial frames of reference is provided based on a Doppler effect analysis. A cinematic equation describing the motion in a medium excited by a moving source is derived
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29

Rangappa, Pradeep, and Ipe Jacob. "Pioneer of the Doppler Effect." Journal of Acute Care 2, no. 3 (February 19, 2024): 168–69. http://dx.doi.org/10.5005/jp-journals-10089-0092.

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30

Čojanović, Miloš. "Derivation of general Doppler effect equations." JOURNAL OF ADVANCES IN PHYSICS 18 (December 2, 2020): 150–57. http://dx.doi.org/10.24297/jap.v18i.8913.

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In this paper, we will derive the general equations for Doppler effect. It will be proved that regardless of the nature of the emitted waves and the medium through which the waves propagate the formula always has the same form and is identical to the general Doppler effect formula for sound. We will also show that Doppler effect can be used to establish a relationship between the local time of the source and the local time of the receiver. In addition, some new characteristics of the Doppler effect have been presented that have not been discussed in the literature so far.
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31

Choi, Yang-Ho. "Systematic approach to the relativistic Doppler effect based on a test theory." Canadian Journal of Physics 94, no. 10 (October 2016): 1064–70. http://dx.doi.org/10.1139/cjp-2016-0340.

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Numerous experiments have been carried out to validate the Lorentz transformation or to find possible violations of Lorentz invariance, based on test theories to test special relativity. The test theory of Mansouri and Sexl (MS) provides a general framework for the transformation of inertial frames, presuming a preferred system of reference. Based on the MS framework, this paper systematically approaches the relativistic Doppler effect such that its dependency on transformation coefficients and parameters can be investigated. The Doppler effect is formulated in a complex Euclidean space where time is represented with imaginary numbers. Two formulae of the Doppler effect, which have been derived in an arbitrary transformation within the MS framework, are presented: one between an inertial frame and the preferred one and the other between arbitrary inertial frames. It is shown from the former formulation that the Doppler effect is independent of the synchronization of clocks, which implies that the Doppler-shifted frequency in the absolute synchronization is the same as that in the standard synchronization. The latter formula can allow us to find Doppler shifts without information on the velocities of inertial frames relative to the preferred frame. Exploiting these theoretical results, we examine the transverse and the longitudinal Doppler effects in detail.
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32

Dragoset, William H. "Marine vibrators and the Doppler effect." GEOPHYSICS 53, no. 11 (November 1988): 1388–98. http://dx.doi.org/10.1190/1.1442418.

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Marine seismic data acquired with a moving vibrator suffer phase dispersion caused by Doppler shifting of the source sweep function. The dispersion for a particular reflection event depends upon frequency, the type of sweep function, and the Doppler factor associated with that event. Synthetic vibrator data show that, at typical ship speeds, the Doppler factors for steeply dipping events are big enough to cause phase dispersion as large as several hundred degrees. If unaccounted for, such dispersive effects could make a moving marine vibrator unacceptable for imaging steep dips. In a constant‐offset section, the Doppler factor for a reflection event is the product of ship speed and the event’s time dip. That key, simple relationship allows a two‐dimensional f-k filter to remove the phase dispersion caused by the Doppler effect. Comparisons of both synthetic data and Gulf of Mexico field data, before and after application of the phase‐correcting filter, show that the filter improves steep‐dip imaging in marine vibrator data. For the Gulf of Mexico line, steep dips are imaged just as well in the phase‐corrected vibrator data as in air‐gun data.
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33

Malik, Adam, Widiastuti Ledgeriani Mugiri, Rizki Zakwandi, Sani Safitri, and Tia Juliani. "Simple Experiment of Doppler Effect Using Smartphone Microfon Sensor." Jurnal Penelitian Fisika dan Aplikasinya (JPFA) 10, no. 1 (May 22, 2020): 1. http://dx.doi.org/10.26740/jpfa.v10n1.p1-10.

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Doppler effect is the physical phenomena in which the emitted frequency is a source of change at a time when accepted by the detector due to relative movement of the detector towards the source of the wave or vice versa. This research aims to identify the Doppler effect symptoms by utilizing sensors found in smartphones. This research uses experimental method that combine the mechanical instruments and microphone smartphone sensor as measurement tool. The mechanical instruments used are a smartphone with the help of frequency sound generator software, Physics Toolbox, the camera as an instrument of data collectors, and Tracker as a motion analyzer software. Based on the results of the experiments, the author retrieved the value of the error and the standard deviation of each of the observed symptoms. The symptoms of Doppler effect upon source moving closer and moving away when the silent observer shows the error value of 0.04 % and 0.1185 % respectively with a standard deviation of 0.018 and 1.005. In addition, the experiment on Doppler effect as the source is staying still and as the observer approaching the source provides error value of 8.60 % and standard deviation of 13.501. As for the experiment on Doppler effect as the source and the observers are approaching each other displays the error value of 4.31 % and the standard deviation of 0.087. Overall, this experiment generates error value of 3.267 % and standard deviation of 3.665, inferring that the experiments conducted are accurate and precise in representing the Doppler effect phenomenon. Based on the results of this experiments, the researcher recommends to carry out practicum on Doppler effects with the help of smartphone sensors.
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34

Lu, Yan, Siwei Kou, and Xiaopeng Wang. "Micro-Doppler Effect and Sparse Representation Analysis of Underwater Targets." Sensors 23, no. 19 (September 25, 2023): 8066. http://dx.doi.org/10.3390/s23198066.

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At present, the micro-Doppler effects of underwater targets is a challenging new research problem. This paper studies the micro-Doppler effect of underwater targets, analyzes the moving characteristics of underwater micro-motion components, establishes echo models of harmonic vibration points and plane and rotating propellers, and reveals the complex modulation laws of the micro-Doppler effect. In addition, since an echo is a multi-component signal superposed by multiple modulated signals, this paper provides a sparse reconstruction method combined with time–frequency distributions and realizes signal separation and time–frequency analysis. A MicroDopplerlet time–frequency atomic dictionary, matching the complex modulated form of echoes, is designed, which effectively realizes the concise representation of echoes and a micro-Doppler effect analysis. Meanwhile, the needed micro-motion parameter information for underwater signal detection and recognition is extracted.
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35

LU, Jun, Qunfei ZHANG, Wentao SHI, and Lingling ZHANG. "Doppler estimation and compensation method for underwater target active detection based on communication signal." Xibei Gongye Daxue Xuebao/Journal of Northwestern Polytechnical University 39, no. 5 (October 2021): 962–70. http://dx.doi.org/10.1051/jnwpu/20213950962.

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The integration of underwater detection and communication uses communication signals to detect a target actively, but the Doppler effect deteriorates the parameter estimation performance of the integrated system. To eliminate the influence of the Doppler effect, a joint Doppler estimation and compensation method based on spectrum zooming and correction is proposed. Firstly, the synchronization signal is used to obtain the signal receiving delay and intercept the single-frequency signal segment in the received signal. Then, the discrete Fourier transform is used to find the frequency that corresponds to the maximum amplitude of the single-frequency signal segment. Finally, the frequency spectrum is refined and corrected within the range near the frequency. The Doppler factor is estimated and the received signal is compensated by the Doppler estimation value. The simulation results show that the proposed method improves Doppler factor estimation accuracy, increases the cross-correlation processing gain and improves DOA (direction of arrival) estimation performance, thus being robust to different Doppler effects.
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36

Huang, Y. S., and K. H. Lu. "Formulation of the classical and the relativistic Doppler effect by a systematic method." Canadian Journal of Physics 82, no. 11 (November 1, 2004): 957–64. http://dx.doi.org/10.1139/p04-049.

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The classical and the relativistic Doppler effect for both acoustic and light waves are formulated exactly by a systematic method. This method differs only in its usage of classical and relativistic transformation laws in the formulation of the classical and relativistic Doppler effect, respectively. The method is straightforward, and much more logically rigorous than the typical demonstrations using graphical illustration. In the formulation of the classical Doppler effect, as expected, no aberration and no transverse classical Doppler effect are found. In the formulation of the relativistic Doppler effect, one important discovery is that the transverse relativistic Doppler effect depends only on the speed of the source relative to the observer, irrespective of the nonskew velocities of the source and the observer relative to the medium. PACS No.: 03.30.+p
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37

Maier, V. V., and R. V. Maier. "Demonstration of the acoustic Doppler effect." Uspekhi Fizicheskih Nauk 161, no. 3 (1991): 149–53. http://dx.doi.org/10.3367/ufnr.0161.199103h.0149.

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38

Polupanov, V. N. "Transverse Doppler Effect-Based Frequency Shifter." Telecommunications and Radio Engineering 65, no. 7 (2006): 589–93. http://dx.doi.org/10.1615/telecomradeng.v65.i7.10.

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39

Kobayashi, H. "Ultrasonic ground speedometer utilizing Doppler effect." Journal of the Acoustical Society of America 94, no. 4 (October 1993): 2468. http://dx.doi.org/10.1121/1.407433.

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40

Hughes, Stephen W., and Michael Cowley. "Teaching the Doppler effect in astrophysics." European Journal of Physics 38, no. 2 (January 16, 2017): 025603. http://dx.doi.org/10.1088/1361-6404/aa5446.

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41

Ran, Jia, Yewen Zhang, Xiaodong Chen, and Hong Chen. "Frequency Mixer Based on Doppler Effect." IEEE Microwave and Wireless Components Letters 28, no. 1 (January 2018): 43–45. http://dx.doi.org/10.1109/lmwc.2017.2772344.

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42

Peres, Asher, and Daniel R. Terno. "Relativistic doppler effect in quantum communication." Journal of Modern Optics 50, no. 6-7 (April 2003): 1165–73. http://dx.doi.org/10.1080/09500340308234560.

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43

Li, Guixin, Thomas Zentgraf, and Shuang Zhang. "Rotational Doppler effect in nonlinear optics." Nature Physics 12, no. 8 (March 21, 2016): 736–40. http://dx.doi.org/10.1038/nphys3699.

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44

Rosanov, N. N. "Parametric doppler effect for laser pulses." Optics and Spectroscopy 109, no. 1 (July 2010): 133–35. http://dx.doi.org/10.1134/s0030400x10070222.

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45

Seddon, N. "Observation of the Inverse Doppler Effect." Science 302, no. 5650 (November 28, 2003): 1537–40. http://dx.doi.org/10.1126/science.1089342.

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46

Bertotti, Bruno. "Doppler Effect in a Moving Medium." General Relativity and Gravitation 30, no. 2 (February 1998): 209–26. http://dx.doi.org/10.1023/a:1018892610774.

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47

Gusakov, E. Z., A. V. Surkov, and A. Yu Popov. "Multiple scattering effect in Doppler reflectometry." Plasma Physics and Controlled Fusion 47, no. 7 (May 31, 2005): 959–74. http://dx.doi.org/10.1088/0741-3335/47/7/001.

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48

Maĭer, V. V., and R. V. Maĭer. "Demonstration of the acoustic Doppler effect." Soviet Physics Uspekhi 34, no. 3 (March 31, 1991): 262–64. http://dx.doi.org/10.1070/pu1991v034n03abeh002354.

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49

Nepomnyashchy, Y. A. "Unusual Doppler effect in He II." Physical Review B 47, no. 2 (January 1, 1993): 905–14. http://dx.doi.org/10.1103/physrevb.47.905.

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50

Rossing, Thomas D. "The doppler effect and racing cars." Physics Teacher 26, no. 7 (October 1988): 423. http://dx.doi.org/10.1119/1.2342560.

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