
fig 1
It is important to remeber that it is not a photo, but a mathematical model based on our understanding of rock and wave physics. This means it is not perfect.
The model may exhbit a "bright" spot where the signal returned from the sub surface changes significantly on the displayed section. These can often be caused by a gas reservoir. The gas in the rocks strongly effects how the waves travel and how they return to surface. In figure 2 below we see the amplituides at 1.4 and 1.6 get stronger as we move right to left and then die off again. This may indicate a reservoir. Each second on the diagram correspods to 5000'.

fig 2
Unfortunately often might not even be 50% of the time and drilling every bright spot means a lot of dry holes being drilled. Obviously this is not what we want, drilling a hole 3km into the surface is an expensive prospect.
In figure 1 we would see a difference in amplitude between the two rays despite the fact they are reflecting from the same point, this is caused by the different angle the rays strike the reflector at. As mentioned earlier, summing these or stacking them removes this information but produces a good signal of that point. The formulas for this relationship are complex and have been simplified over time. A simplifictaion by Shuey is the most common way to express this relationship.
Analyzing how the relationship of how the amplitudes change with incidence angle can answer some important questions. Do we see the amplitudes getting weaker as we move further from the source? Or do we see them getting stronger?
In general the responses can be classified in 4 ways and will tell us what type of rock and what type of fluid we have in the pores.
This is the basic idea behind AVO and a formation charged with gas will exhbit a different AVO response than one charged with water. And more importantly it can be used to differeniate a gas charged bright spot from another anomaly.
This gives us a basic understanding of AVO and a place to move forward from.
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