Fraunhofer zone is another name for far field in telecommunications. It is an area where antenna signal looses its resolution.
if we're talking about a short dipole, you have {E.H} field depending by r^(-k), where r is distance between antenna's feed and point of {E,H} calculus and k is >=1. In far field, you can imagine r>>1, so r^(-k) contribution is lower for greater k and you can approximate {E,H} expression by considering only the contribution with the lowest k. This make Poynting vector become real, according with the assumption that far field radiation power is active, near field one has also a capacitive contribution.
According to Faraday's law: "When current is passed through a conductor, an EM field is produced surrounding it." As an antenna contains one or more conductors, the terminals of which are connected to some voltage, when this voltage at the terminals is applied, it produces/induces the alternating current which radiates the elements in the electromagnetic field. (Transmission) The reverse of this occurs in reception; where the electromagnetic field from another source induces an alternating current in the antenna, and a corresponding voltage at the antenna's terminals.
Because there is an electrostatic field in that region of space
Faraday's Law
Fraunhofer zone is another name for far field in telecommunications. It is an area where antenna signal looses its resolution.
Rephrase the question, What antenna?
Its is at the ski mountain
the far north region
Its on ski hill
The RFID is powered by its own antenna. When in the presence of a pulating magnetic field, the antenna generates a signal that can power up the RFID, causing it to generate its code on top of that field.
Yes, you certainly can. But the car antenna probably won't work as efficiently as one that's specifically designed for CB. That means you probably won't be able to hear as far or talk as far as you could if you used the right antenna.
yes
if we're talking about a short dipole, you have {E.H} field depending by r^(-k), where r is distance between antenna's feed and point of {E,H} calculus and k is >=1. In far field, you can imagine r>>1, so r^(-k) contribution is lower for greater k and you can approximate {E,H} expression by considering only the contribution with the lowest k. This make Poynting vector become real, according with the assumption that far field radiation power is active, near field one has also a capacitive contribution.
The antenna should be parallel to the electrostatic field of the wave, and perpendicular to its magnetic field and to its direction of propagation.
All types... depending on frequency and application. Lower frequency RFID's are typically near field and use inductive antenna designs, higher frequency ones use far-field designs. Low frequency RFID's like the TIRIS pet ID's use coils of wound wire. HF type RFID's like MiFARE use simple planar loop antenna designs. Most VHF RFID's use dipole and modified dipole designs with reflector elements. UHF and microwave RFID's frequently use patch and slot antenna designs.
The fastest traveling wave is the transverse wave of electromagnetic radiation. Along the radiating antenna, it travels at the speed of light. There are two velocity components in space: one is the radial component, which also travels at the speed of light. The other is the transverse velocity component, which increases with distance. In the far, far field, it is much greater than the speed of light. The characteristics of the antenna electromagnetic dynamic field waves were plotted directly from the well known radiation equation,