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This section provides an overview of the phenomena known as Fresnel Effect or Fresnel Zones. Since Monsieur Fresnel was a French physicist/mathematician drop the 's' when pronouncing his name to show you are real savvy (or should that be 'chic').
Bad News: If you can see the receiving antenna the wireless link still might not work - this is entirely the fault of M. Fresnel (aided and abetted by a few natural laws). If you prefer some action ("to !#? with the theory just gimme the numbers") go direct to our Fresnel Calculator.
Here goes for a quick explanation of the problem (with suitable apologies for the superficiality). Direct radio waves will obviously travel in a straight line from the transmitter (TX) to the receiver (RX). But remember there are other waves travelling out inside the signal 'cone' (or circle if the antenna is a omni). If these other waves don't bump into anything (there are no obstacles) they will just travel off into the night until overcome with exhaustion. But if they bump into something (a deflection) they may end up at the RX antenna and if they are out of phase with the straight line signals they will have a phase cancelling effect - they will reduce the power of the arriving signal. The magnitude of the phase cancelling effect is a function of the signal strength and how out of phase the signal is (always described in terms of an angle). See diagram 1 below.

Diagram 1 - Phase cancelling effects from deflections (bumps)
Fresnel provided a means to calculate how out of phase the bumps (deflections) between the transmission source (TX) and the receptor (RX) will be. Each Fresnel zone is an ellipsoidal ('sausage like' to the rest of us) shape as shown below. Deflections (bumps) from obstacles which occur anywhere in zone 1 will create signals that will be 0 to 90o out of phase, in zone 2 they will be 90 to 270o out of phase, in zone 3 they will be 270 to 450o out of phase and so on. Even numbered zones are bad'ish (have the maximum phase cancelling effect and odd numbered zones are good'ish (may actually add to the signal power). The signal strength (and hence the magnitude of the phase cancelling effect) is strongest in zone 1 and decreases in each successive zone. At any point which is d1 distance from the TX source and d2 distance from the receptor (RX) each Fresnel zone has a radius value of r1. See diagram 2.

Diagram 2 - Fresnel zones
The big deal is this. To maximise RX strength you need to minimise the effect of the out of phase signals. To do that you must make sure the strongest signals don't bump into anything - they have the maximum chance of getting to the RX location. The strongest signals are the ones closest to the direct line between TX and RX and always lie in the 1st Fresnel Zone. The rule of thumb is that 60% of the 1st Fresnel zone must be clear of obstacles If you have a building, say, that is a distance d1 from the TX antenna and d2 from the RX antenna then it must not be closer than 60% of r1 measured from the centre line of sight (c1 in diagram). You may need to juggle the antenna positioning to ensure this 60% zone is clear (you will also see this 60% figure written as 0.6 just to confuse). See diagram 3.

Diagram 3 - Fresnel zone clearance
Finally on longer links especially (> 3Km or 2 miles) you will frequently see discussions about Fresnel zones and the curvature of the earth (though it can have an impact at very much closer distances). The reason - even if you are shooting a link across flat ground with no apparent obstacles, eventually the ground itself becomes the obstacle and can easily get inside the 60% clearance zone. Solution - lift the antenna higher to make sure the earth stays out of your way! In diagram 4 d1 and d2 are the same (the mid point) so the distance of the direct line of sight to the earth (c1) must be more that 60% of r1. Our Fresnel Calculator gives the earth's height (or bulge) at the mid point of the link.

Diagram 4 - Fresnel zone and earth curvature
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