Active Sonar Equation Adapting Passive Ideas Passive Case: LS/ N SL TL NL DI DT From our Sonar TL TL ' 2TL Target Strength describes the fraction of energy reflecting back from the target LS/ N SL 2TL TS NL DI DT Reverberation Noise Reflections from non-target objects is greater that noise. Reverberation limited RL NL DI LS/ N SL 2TL TS RL DT Active Sonar – Materials • Typical piezoelectric materials – Quartz – PZT -Lead zirconate titanate – Barium Titanate Piezoelectricity a a+Da Source Level for an Omnidirectional projector SL 10 log I 1 yd I1 yd I ref p 2rms Pwr c Area at 1 yd where Area at 1 yd 4 1 yd Pwr 2 4π 1 yd 10 log Pwr c SL 10 log 2 p 2ref 4 1 yd p 2ref c 1000 kg/m 1500 m/s SL 10 log Pwr 10 log 4 1 yd 0.9144 m 1x10 1 yd 3 2 2 6 Pa 2 10 log Pwr 171.5 dB 2 Electrical Efficiency PwrElectric Pwracoustic PwrElectric E where E is the system efficiency thus: SL 171.5 dB 10 log PE E Pwracoustic SL 171.5 dB 10 log PE 10 log E Efficiency may range from 20% to 70% for most sonar applications Directional Arrays DI T 10 log I non directional I directional Principle of Reciprocity b , receiving b , Transmitting SL 171.5 dB 10log PE 10log E DIT Transducer Sensitivity How many dB for 1 volt input? I SV 10log 1V Iref p1V 20log p ref V2 PE R SL @1V SV 171.5 10log R P 10log E DI Input impedance Manufacturers typically advertise based on SV. To find SL, add 20logV. Example • Compute the source level for an circular piston projector of diameter = 1 meter radiating 10 kW acoustic power at a frequency of 15 kHz in water SL 171.5 dB 10log PE 10log E DIT 1m D DIT 10 log 29.94dB 10 log .1m 2 Piston array: 2 SL 171.5 dB 10log104 29.94 dB 241.5 dB Cavitation Pressure Threshold Power Threshold pcav patm 104 z Pcav S pcav (z in meters) 2 2 c S = Tranducer Surface Area SLcav 186 10log S DI 20log 10 z