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Ultrasonic Sound Properties. Examples of oscillation ball on a spring pendulum rotating earth.

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Presentation on theme: "Ultrasonic Sound Properties. Examples of oscillation ball on a spring pendulum rotating earth."— Presentation transcript:

1 Ultrasonic Sound Properties

2 Examples of oscillation ball on a spring pendulum rotating earth

3 The ball starts to oscillate as soon as it is pushed Pulse

4 Oscillation

5 Movement of the ball over time

6 Time One full oscillation T Frequency From the duration of one oscillation T the frequency f (number of oscillations per second) is calculated: 1/T = f

7 18036090270 Phase Time a 0 The actual displacement a is termed as:

8 Spectrum of sound Frequency range HzDescription Example 0 - 20 Infrasound Earth quake 20 – 20,000 Audible soundSpeech, music > 20,000 Ultrasound Bat, Quartz crystal

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10 gas liquid solid Atomic structures low density weak bonding forces medium density medium bonding forces high density strong bonding forces crystallographic structure

11 Ultrasonic Sound Properties Sound waves used in most engineering applications are longitudinal waves. These mechanical waves can propagate in solids, liquids, and gases. The waves originate at a vibration source and move through a medium by material particles oscillating in the direction of the propagation of the wave. Electromagnetic waves are affected by the phenomena of reflection, refraction, diffraction, absorption, polarization and scattering. Wave propagation is any of the ways in which waves travel.

12 Understanding wave propagation: Spring = elastic bonding forceBall = atom

13 T distance travelled start of oscillation

14 T Distance travelled From this we derive speed of wave through the medium (c): or Wave equation During one oscillation T the wave front propagates by the distance :

15 Longitudinal waves, also known as "l-waves", are waves that have the same direction of vibration as their direction of travel, which means that the movement of the medium is in the same direction as or the opposite direction to the motion of the wave. Mechanical longitudinal waves have been also referred to as compressional waves or compression waves.

16 Direction of oscillation Direction of propagation Longitudinal wave Sound propagation

17 A transverse wave is a moving wave that consists of oscillations occurring perpendicular (or right angled) to the direction of energy transfer. If a transverse wave is moving in the positive x-direction, its oscillations are in up and down directions that lie in the y–z plane.

18 Direction of propagation Transverse wave Direction of oscillation Sound propagation

19 A light wave is an example of a transverse wave. Plane pressure pulse wave. transverse wavelongitudinal waves

20 Wave propagation Air Water Steel, long Steel, trans 330 m/s 1480 m/s 3250 m/s 5920 m/s Longitudinal waves propagate in all kind of materials. Transverse waves only propagate in solid bodies. Due to the different type of oscillation, transverse waves travel at lower speeds. Sound velocity mainly depends on the density and E- modulus of the material.

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22 Reflection and Transmission As soon as a sound wave comes to a change in material characteristics, e.g. the surface of a workpiece, or an internal inclusion, wave propagation will change too:

23 Behaviour at an interface Medium 1Medium 2 Interface Incoming wave Transmitted wave Reflected wave

24 Reflection + Transmission: Perspex - Steel Incoming wave Transmitted wave Reflected wave PerspexSteel 1,87 1,0 0,87

25 Reflection + Transmission: Steel - Perspex 0,13 1,0 -0,87 Perspex Stee l Incoming wave Transmitted wave Reflected wave

26 Amplitude of sound transmissions: Strong reflection Double transmission No reflection Single transmission Strong reflection with inverted phase No transmission Water - Steel Copper - SteelSteel - Air

27 The use of ultrasonic waves has primarily focused on two wave properties: speed of sound and attenuation. In addition, the Doppler frequency shift effect provides information in systems that involve fluid motion.

28 Application: speed of sound For some food systems, the speed of sound alone can be used to measure various physical properties. Speed of sound has been considered an accurate index for determining the concentration, composition and temperature of aqueous solutions. Contreras et al. studied the relation between speed of sound of sugar solutions with concentration and temperature and summarized the results with an empirical equation.

29 Application: attenuation In some food systems, ultrasonic attenuation is a more useful property than measurements of sound velocity. Attenuation indicates the energy loss of the sound waves during transmission in a medium. Gladwell et al. characterized the rheological properties of edible oil using ultrasonic attenuation behavior. The radius of the droplets in an emulsion can be measured by studying the attenuation based on ultrasonic scattering theories. This can be applied to evaluate the milk homogenization process.

30 Cavitation Cavitation is the formation and then immediate implosion of cavities in a liquid – i.e. small liquid-free zones ("bubbles") – that are the consequence of forces acting upon the liquid. It usually occurs when a liquid is subjected to rapid changes of pressure that cause the formation of cavities where the pressure is relatively low. Cavitation is a significant cause of wear in some engineering contexts. When entering high pressure areas, cavitation bubbles that implode on a metal surface cause cyclic stress. 2 types: Stable and Transient cavitation

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33 Liquid driven transducer

34 Magnetostrictive transducer Electrical energy  mechanical energy by magnetostriction from ferromagnetic materials (Ni, Fe) that occur dimension change in magnetic field (continuous change  cause of oscillation  produce low frequency of ultrasound).

35 Piezoelectric transducer Use ceramics that consist of piezoelectric materials (barium titanate, lead metaniobate)

36 Piezoelectric Effect Piezoelectrical Crystal (Quartz) Battery +

37 + The crystal gets thicker, due to a distortion of the crystal lattice Piezoelectric Effect

38 + The effect inverses with polarity change Piezoelectric Effect

39 An alternating voltage generates crystal oscillations at the frequency f U(f) Sound wave with frequency f Piezoelectric Effect

40 A short voltage pulse generates an oscillation at the crystal‘s resonant frequency f 0 Short pulse ( < 1 µs ) Piezoelectric Effect

41 Reception of ultrasonic waves A sound wave hitting a piezoelectric crystal, induces crystal vibration which then causes electrical voltages at the crystal surfaces. Electrical energy Piezoelectrical crystal Ultrasonic wave

42 Ultrasonic baths (40 kHz)

43 Cup horn type

44 Ultrasonic probe systems Transducer + horn Horn

45 Ultrasonic probe systems

46 ultrasonic measurement system

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48 Ultrasound Techniques Cause of direct oscillation : use in surface cleaning The pulse-echo ultrasound: A pulsed-echo system utilizes the echo of the transmitted sound waves to characterize the sample. A single transducer both transmits the sound waves and receives the echo in this system.

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50 c = speed of sound d = distance that sound travels t = time A 1 = amplitude of the first echo A i = amplitude of the incident wave R = reflection coefficient

51 Since R(air) ≈1 (i.e., no sample is in the sample holder), Z 1 and Z 2 = acoustic impedances of the material the wave is traveling through and the reflecting material, respectively.

52 Acoustic impedance (Z) is defined as the wave pressure over the particle velocity. For a wave in a weakly absorbing medium the acoustic impedance can be written:

53 Ultrasound Techniques The Doppler effect : the echoes The basis of ultrasonic Doppler velocimetry (UDV) techniques is that reflected/scattered ultrasonic waves from a moving interface undergo a frequency shift.

54 The measurement of a flow velocity is based on detecting the Doppler effect of the propagated ultrasound waves due to the fluid movement. There are two types of UDV: a continuous- wave Doppler system and a pulse-wave Doppler system. The pulse system is more commonly used in engineering applications.

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56 Application in food industry Oxidation process: accelerate of aging process of wine using 1 MHz. Enzyme reactions: to reduce peroxidase activity by using 20 kHz at 371 W/cm 2

57 stimulation of living cells : use in fermentation Sterilization process: use for surface decontamination

58 ultrasonic emulsification Extraction meat products: apply to extract protein by salt solution (ultrasound can use to destroy myofibrils in tissue and connective tissues to obtain more soft tissues) Crystallization: accelerate nucleation rate and crystal growth Degassing of liquids: cavitation Acoustically aided filtration: agglomeration of fine particles Acoustic drying: combination with drying to reduce drying temp. Defoaming

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60 Sound reflection at a flaw Probe Flaw Sound travel path Work piece s

61 Plate testing delamination plate 0246810 IP F BE IP = Initial pulse F = Flaw BE = Backwall echo

62 0246810 s s Wall thickness measurement Corrosion

63 Through transmission testing 0246810 Through transmission signal 1 2 1 2 T T R R Flaw

64 Weld inspection 020406080100 s a a' d x a = s sinß a' = a - x d' = s cosß d = 2T - t' s Lack of fusion Work piece with welding F ß = probe angle s = sound path a = surface distance a‘ = reduced surface distance d‘= virtual depth d = actual depth T= material thickness ß

65 Straight beam inspection techniques: Direct contact, single element probe Direct contact, dual element probe Fixed delay Immersion testing Through transmission

66 surface = sound entry backwall flaw 12 water delay 0 246810 0 2468 IE IP BE F 1 2 Immersion testing


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