RU96121682A - METHOD FOR DETERMINING SOUND SPEED DISTRIBUTION IN LIQUID MEDIA - Google Patents

METHOD FOR DETERMINING SOUND SPEED DISTRIBUTION IN LIQUID MEDIA

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Publication number
RU96121682A
RU96121682A RU96121682/28A RU96121682A RU96121682A RU 96121682 A RU96121682 A RU 96121682A RU 96121682/28 A RU96121682/28 A RU 96121682/28A RU 96121682 A RU96121682 A RU 96121682A RU 96121682 A RU96121682 A RU 96121682A
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RU
Russia
Prior art keywords
points
reception
acoustic
acoustic signals
receiving
Prior art date
Application number
RU96121682/28A
Other languages
Russian (ru)
Inventor
Н.Н. Касьяненко
Г.Н. Серавин
Original Assignee
Н.Н. Касьяненко
Г.Н. Серавин
Filing date
Publication date
Application filed by Н.Н. Касьяненко, Г.Н. Серавин filed Critical Н.Н. Касьяненко
Publication of RU96121682A publication Critical patent/RU96121682A/en

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Claims (4)

1. Способ определения распределения скорости звука в жидкой среде, заключающийся в зондировании из точки излучения акустическими сигналами расположенных в жидкой среде акустических отражателей, приеме отраженных от них акустических сигналов в первой, второй и третьей точках приема, причем первая точка приема совмещена с акустическим источником, а вторая и третья точки приема удалены от него на фиксированные расстояния, измерении времен распространения акустических сигналов от точки излучения до точек отражения и далее к точкам приема, нахождения по их значениям с учетом известных расстояний от акустического источника до точек приема искомого параметра, отличающийся тем, что дополнительно производят прием отраженных акустических сигналов по крайней мере в четвертой точке приема, которую располагают на одной линии с первой, второй и третьей точками приема, по временам распространения акустических сигналов от точек отражения до точек приема, известным расстоянием между точками приема акустических сигналов находят углы прихода акустических сигналов к точкам приема и с их учетом определяют значения скорости звука в жидкости у акустических отражателей и их вертикальные координаты.1. The method of determining the distribution of sound velocity in a liquid medium, which consists in sensing acoustic reflectors located in the liquid medium from the point of emission with acoustic signals, receiving acoustic signals reflected from them at the first, second and third reception points, the first receiving point being combined with an acoustic source, and the second and third reception points are removed from it at fixed distances, measuring the propagation times of acoustic signals from the radiation point to the reflection points and further to the reception points, finding according to their values, taking into account the known distances from the acoustic source to the reception points of the desired parameter, characterized in that they additionally receive reflected acoustic signals at least at the fourth reception point, which is located on the same line with the first, second and third reception points, according to the propagation times of the acoustic signals from the reflection points to the receiving points, the angles of arrival of the acoustic signals to the receiving points are found by the known distance between the receiving points of the acoustic signals and taking them into account, the values of the speed of sound in the liquid at the acoustic reflectors and their vertical coordinates are determined. 2. Способ по п. 1, отличающийся тем, что точки приема акустических сигналов расположены по одну сторону от акустического источника. 2. The method according to p. 1, characterized in that the points of reception of acoustic signals are located on one side of the acoustic source. 3. Способ по п. 2, отличающийся тем, что углы прихода принятых акустических сигналов в точки приема находят по формулам
Figure 00000001

Здесь φ1i, φ2i и φ3i - угол прихода акустического сигнала от i-го отражателя к первой, второй и третьей точкам приема, начиная с самой удаленной от точки излучения;
Figure 00000002

Figure 00000003

Figure 00000004

τ12 = t1i - t2i;
τ23 = t2i - t3i;
τ13 = t1i - t3i;
t1i, t2i и t3i - время распространения акустического сигнала от i-го отражателя соответственно к первой, второй и третьей точкам приема, начиная с самой удаленной от точки излучения;
t01, t02 и t03 - время распространения акустического сигнала между первой и второй, второй и третьей, первой и третьей точек приема соответственно.
3. The method according to p. 2, characterized in that the angles of arrival of the received acoustic signals at the receiving points are found by the formulas
Figure 00000001

Here φ 1i , φ 2i and φ 3i - the angle of arrival of the acoustic signal from the i-th reflector to the first, second and third points of reception, starting from the farthest from the radiation point;
Figure 00000002

Figure 00000003

Figure 00000004

τ 12 = t 1i - t 2i ;
τ 23 = t 2i - t 3i ;
τ 13 = t 1i - t 3i ;
t 1i , t 2i and t 3i - propagation time of the acoustic signal from the i-th reflector to the first, second and third points of reception, respectively, starting from the farthest from the radiation point;
t 01 , t 02 and t 03 - propagation time of the acoustic signal between the first and second, second and third, first and third points of reception, respectively.
4. Способ по п. 2, отличающийся тем, что значение скорости звука сi на горизонтах zi акустических отражателей в жидкой среде с постоянным градиентов скорости звука находят по формулам
Figure 00000005

zi = D3tgφ3i;
dik = Di - Dk;
Figure 00000006

сi(zi) - значение сокрости звука i-го отражателя, расположенного на горизонте zi;
i,k - номера точек приема при i = 1, k = 2, 3; i = 2, k = 3;
dik - расстояние между соответствующими точками приема;
Di, Dk - расстояния между точкой излучения и точками приема.
4. The method according to p. 2, characterized in that the value of the speed of sound with i at the horizons z i of acoustic reflectors in a liquid medium with constant gradients of the speed of sound is found by the formulas
Figure 00000005

z i = D 3 tgφ 3i ;
d ik = D i - D k ;
Figure 00000006

with i (z i ) is the value of the soundness of the sound of the i-th reflector located on the horizon z i ;
i, k are the numbers of reception points for i = 1, k = 2, 3; i = 2, k = 3;
d ik is the distance between the corresponding points of reception;
D i , D k - the distance between the radiation point and the receiving points.
RU96121682/28A 1996-11-06 METHOD FOR DETERMINING SOUND SPEED DISTRIBUTION IN LIQUID MEDIA RU96121682A (en)

Publications (1)

Publication Number Publication Date
RU96121682A true RU96121682A (en) 1999-01-20

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2456554C2 (en) * 2010-07-20 2012-07-20 Игорь Иванович Микушин Method of measuring distribution of sound speed in liquid medium
RU2515125C1 (en) * 2012-11-30 2014-05-10 Открытое акционерное общество "Концерн "Океанприбор" Method of determining sound speed
RU2631234C1 (en) * 2016-07-01 2017-09-19 Акционерное Общество "Концерн "Океанприбор" Method of determining sound speed

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2456554C2 (en) * 2010-07-20 2012-07-20 Игорь Иванович Микушин Method of measuring distribution of sound speed in liquid medium
RU2515125C1 (en) * 2012-11-30 2014-05-10 Открытое акционерное общество "Концерн "Океанприбор" Method of determining sound speed
RU2631234C1 (en) * 2016-07-01 2017-09-19 Акционерное Общество "Концерн "Океанприбор" Method of determining sound speed

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