Wideband multifrequency acoustic transducer

• US 5,706,252 A
• Filed: 01/06/1997
• Issued: 01/06/1998
• Est. Priority Date: 07/08/1994
• Status: Expired due to Term

• Current Assignee: Thomson-CSF
• Original Assignee: Thomson-CSF
• Inventors: Le Verrier, Bertrand, Roux, Gerard, Tardy, Bruno, Ramos, Alphonse
• Primary Examiner(s): Eldred, J. Woodrow
• Application Number:
  US08/750,862
• Time in Patent Office: 365 Days
• Field of Search: 367/152, 367/157, 367/162, 367/151, 310/334, 310/335, 310/337
• US Class Current: 367/152
• CPC Class Codes: B06B 1/0614 for generating several frequencies
• CPC Class Codes: B06B 1/0644 using a single piezoelectric element B06B1/0688 takes precedence

Abstract

The invention relates to multifrequency acoustic transducers exhibiting a wide band around each resonant frequency. It consists in inserting between a λ/2 active emitter plate (201) and the soft reflector (203) which supports it a rear plate (202) resonating in λ/4 mode and in placing on this active plate two marcher plates (204, 205) whose impedances are designed so as to best match the two frequencies obtained by inserting this rear plate. Thicknesses of these marcher plates are optimized with the aid of a model of for example Mason type starting from a value close to λ/4 for the frequency to be matched. It makes is possible to construct sonar transducers which operate equally well in detection mode and in classification mode.

Claims

1. Wideband multifrequency acoustic transducer, of the type comprising a piezoelectric emitter plate (201) of impedance Z and resonating in λ

/2 mode at a fundamental frequency F0, a rear plate (202) of impedance Z3 and a support (203) forming a reflector of the type with substantially zero impedance, characterized in that the rear plate (202) resonates in λ

/4 mode at the frequency F0 so as to make it possible to obtain two resonant frequencies FA and FB of the assembled transducer, and in that this transducer furthermore comprises two front marcher plates (204,

     205) whose impedances Z1 and Z2 are given by the formulae

space="preserve" listing-type="equation">Z1≅

Z0.sup.3/5 ×

Z.sup.2/5

space="preserve" listing-type="equation">Z2≅

Z0.sup.2/5 ×

Z.sup.3/5

and whose thicknesses enable them to resonate at frequencies substantially equal to λ

/4 for respectively each of the frequencies FA and FB and to be substantially transparent for respectively each of the other frequencies;

these thicknesses being optimized with the aid of a Mason type model.

2. Transducer according to claim 1, characterized in that the rear plate (202) is formed from the same material as the active plate (201).

3. Transducer according to claim 2, characterized in that the material constituting the active layer (201) and the rear plate (202) is a ceramic of the PZT type for which Z is substantially equal to 21×

10⁶ acoustic ohms, in that the marcher plates (204,

     205) have respective impedances Z1=3.9×

10⁶ acoustic ohms and Z2=6×

10⁶ acoustic ohms, and in that the thicknesses of these plates are respectively equal as a function of the wave frequency which they are required to match to e1=λ

/2.16 and e2=λ

/5.04 at the 1st frequency, and to e1=λ

/3.77 and e2=λ

/8.81 at the 2nd frequency.

4. Transducer according to claim 4, characterized in that the active plate (201) has a thickness such that it resonates in λ

/2 mode at a frequency of 250 kHz and in that the two frequencies of emission for which the transducer is matched are substantially equal to 350 kHz and 150 kHz.