rayleigh_distance
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| rayleigh_distance [2025/06/02 19:38] – created np | rayleigh_distance [2025/06/02 19:41] (current) – created np | ||
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| - | ==== Transmitting distance for acoustic and RF based WPT ==== | ||
| The transmitting distance can be divided into three distinct zones, based on the distance from the source and the behaviour of the acoustic wave. | The transmitting distance can be divided into three distinct zones, based on the distance from the source and the behaviour of the acoustic wave. | ||
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| === (Reactive) Near-field zone === | === (Reactive) Near-field zone === | ||
| - | The near-field or also called the reactive zone lies very close to the surface of the transmitting transducer, typically within one wavelength. In this region, the pressure and particle velocity are not in phase and standing wave effects dominate. This means that the energy is mostly stored and not radiated. In this situation, the receiver must be tightly coupled or directly in contact with the source to transfer power [14], [15]. | + | The near-field or also called the reactive zone lies very close to the surface of the transmitting transducer, typically within one wavelength. In this region, the acoustic |
| === Fresnel zone === | === Fresnel zone === | ||
| - | The Fresnel zone lies beyond the reactive near-field but still before the far-field. It extends up to the Rayleigh distance z, shown in the equation below. This distance marks the end of the region where the waves are highly non-uniform and where interference effects dominate with the beginning of the region where the beam becomes more uniform and spreads out. The equation below shows how to calculate the Rayleigh distance z where D is the diameter of the transducer and λ the wavelength of the energy | + | The Fresnel zone lies beyond the reactive near-field but still before the far-field. It extends up to the Rayleigh distance z, shown in the equation below. This distance marks the end of the region where the waves are highly non-uniform and where interference effects dominate with the beginning of the region where the beam becomes more uniform and spreads out. The equation below shows how to calculate the Rayleigh distance z where D is the diameter of the transducer and λ the wavelength of the acoustic |
| z=2D²/ | z=2D²/ | ||
| - | In this zone, the waves are partially formed and focused energy transfer is possible. It's often the most efficient operating zone for mid-range | + | In this zone, the waves are partially formed and focused energy transfer is possible. It's often the most efficient operating zone for mid-range |
| === Far-field zone === | === Far-field zone === | ||
rayleigh_distance.txt · Last modified: by np