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Calculating amplitude scaler for geometrical spreading correction
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Seismic data wave propagation experiences attenuation of seismic energy due to geometrical spreading, absorption, scattering and due to near surface effects. To recover the loss of energy due to these, we compensate the amplitudes by using various amplitude scaling methods. In one of those methods, we've Spherical Divergence Correction which is mostly happens due to the geometrical spreading.
Spherical divergence correction is applied prior to prestack data to compensate the energy loss (amplitude decay) during the wave propagation. As the wavefront expands the energy is spread over a wider area and the amplitude decays with distance from the source. This amplitude decay is called spherical divergence.
To compensate the amplitude decay, we need to test different combinations of spherical divergence corrections viz., T 2, T 2V and T 2V 2with a single velocity function which is typically "Near surface velocity".
If you choose the offset dependent then the equation will be
• SCALAR (t) = (T * V2/ V0) * SQRT (1 + A) , where
• A = (V2– V02) * X2/ (T02* V4), and
• X = offset of this trace,
• T = trace time at offset X,
• T 0= zero-offset time of this event,
• V = stacking velocity, extracted at time T0,
• V 0= surface velocity (extracted from velocity function at time 0), and we assume that T and T0 are related by the NMO equation:
• T2= T02+ (X/V)2
If we choose the offset independent then the equation will be
A = A0(t)+1/
Where A - corrected amplitude at time t
A0 - Observed amplitude at time t
t - two way travel time
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Offset consideration - When the seismic source like dynamite/vibroseis/air gun fires, the energy penetrates through the sub-surface. During this process the energy is attenuated and dissipated. When the distance(offset) between source and receivers more the energy loss is more. When we consider the offsets in calculating the scalar, then it will consider the t power.

Offset non-consideration - When we consider the offset independent which means, the source-receiver distance (offset) is not a key factor in this calculation. This corrects the amplitude distortion due to the environmental factors and near surface effects. We've consider that the surface wave travel through a constant velocity (near surface velocity) and we've to provide the Time power components.

Time function only - In this case, we are considering the travel time only since the seismic wave propagation happens in homogenous medium.

Apply Correction - This option lets the user to apply the spherical divergence correction to the data.
Remove Correction - In case the input gather has got the spherical divergence correction already applied, we can remove the earlier applied correction by choosing this option.

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In this workflow, we are reading the geometry assigned gathers by using "Read seismic traces" and sorting the data by FFID and Channel as Grouping and Sorting respectively. Inside the seismic loop, we are adding Spherical divergence correction module.

As per the data requirements, test the appropriate parameters. We'll get 4 QC displays for Spherical divergence as shown below. It'll be Input gather, Output gather after spherical divergence correction, Scale factor and Amplitude Graph.

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There are no action items are existing for this module so the user can ignore it.
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YouTube video lesson, click here to open [VIDEO IN PROCESS...]
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Yilmaz. O., 1987, Seismic data processing: Society of Exploration Geophysicist
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