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Piezoelectric Effect
When certain crystals, such as quartz and Rochelle salts, are mechanically vibrated, they produce a voltage. The piezoelectric effect is the name for this action. The crystal phonograph cartridge, for example, is made out of a Rochelle salt crystal to which a needle is attached. The needle swings from side to side as it goes through the grooves of a record. This mechanical motion is applied to the crystal, which results in the generation of a voltage.

Piezoelectricity was discovered by Pierre Curie and his brother Paul Jacques in 1880. When a piezoelectric material is subjected to mechanical stress, it can generate an electric charge. When electricity is applied, however, it begins to vibrate, which is a beneficial property found in a range of items such as gas lighters and speakers. This behaviour is frequently seen in crystalline materials like quartz.

A crystal is typically thought of as a hard structure with atoms arranged in a symmetrical grid-like form, referred to as a unit cell. However, the atoms in piezoelectric crystals are not evenly distributed, but their electric charges are balanced. Squeezing the crystal causes some of the atoms to shift closer and further apart, changing the balance of positive and negative charges and eventually causing an electric current to flow from one end of the crystal to the other. When a voltage is applied to the crystal, the atoms move to rebalance their electric charges, causing the crystal to vibrate.

A piezoelectric sensor is used to make a piezoelectric measurement. This piezoelectric sensor converts changes in force or strain, pressure, acceleration, and temperature to electric charges and monitors them. Piezoelectric sensors can be used to measure a wide range of operations. The following are some significant applications:

Tilt sensor in consumer electronics

Pressure Sensor in the touch pads of mobile phones

Combustion monitoring in internal combustion engines

In Spark plugs of vehicle etc.

Despite the fact that piezoelectric sensors are electromechanical systems that respond to compression, the sensing elements display virtually no deflection. This provides durability, a very high natural frequency, and great linearity over a large amplitude range for piezoelectric sensors. Furthermore, piezoelectric technology is impervious to electromagnetic fields and radiation, allowing for measurements in extreme environments. Some materials, such as gallium phosphate or tourmaline, are particularly stable at high temperatures, allowing sensors to work in temperatures as high as 1000°C. In addition to the piezoelectric action, tourmaline has pyroelectricity.

The capacity to generate an electrical signal when the temperature of a crystal changes is known as pyroelectricity. In piezoceramic materials, this effect is widespread. The fact that piezoelectric sensors cannot be employed for absolutely static measurements is one of their drawbacks. The charge on the piezoelectric material is fixed as a result of a static force. Imperfect insulating materials and a drop in internal sensor resistance in traditional readout electronics result in electron loss and a reduced signal. Internal resistance and sensitivity decline even more at higher temperatures. The main effect of the piezoelectric effect is that the sensitivity decreases as the temperature rises owing to twin formation.

While quartz sensors must be cooled during measurements at temperatures exceeding 300 degrees Celsius, particular forms of crystals, such as GaPO4 galium phosphate, do not form twins until they reach the melting point of the material. It is not true, however, that piezoelectric sensors can only be employed for very quick processes or in low-temperature environments. In reality, many piezoelectric applications provide quasi-static readings, while others operate at temperatures above 500 degrees Celsius. Piezoelectric sensors are also used to detect fragrances in the air by measuring both resonance and capacitance at the same time. Piezoelectric sensors can now be used in a far wider range of applications thanks to computer-controlled electronics. Piezoelectric sensors can be found in nature as well. Some believe that the piezoelectric collagen in bone acts as a biological force sensor.

One of the three major operational modes of a piezoelectric material is determined by the way it is cut:

1.Sheer Effect

The generated charge is proportionate to the applied force and is generated at a right angle to it. The charge is unaffected by the size or shape of the element.

2.Transverse Effect

Charges are displaced in the (x) direction, perpendicular to the force line, when a force is applied along a neutral axis (y). The amount of charge is determined by the geometrical dimensions of the piezoelectric element in question. The transverse effect, unlike the longitudinal and sheer effects, allows for fine tuning of sensitivity based on the applied force and element dimension.

3.Longitudinal Effect

The amount of charge displaced is strictly proportional to the applied force and independent of the piezoelectric element’s size and shape. Putting several elements mechanically ion series and electrically in parallel is the only way to increase the charge output.

The quantity of charge displaced is proportional to the applied force and independent of the size and shape of the piezoelectric element. The only method to enhance the charge output is to connect numerous parts mechanically in series and electrically in parallel.

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One thought on “Piezoelectricity and Piezoelectric Measurements”
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