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|`Mono(i)%npulse`| Integer | Number of pulse cycles |
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|`Mono(i)%support`| Integer | Type of the spatial support of the acoustic source : [1] 1D [2] Finite width (2D) [3] Support for finite line/patch |
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|`Mono(i)%support`| Integer | Type of the spatial support of the acoustic source : [1] 1D [2] Finite width (2D) [3] Support for finite line/patch [4] General support for 3D simulation in cartesian systems [5] Support for monopole acoustic transducer [6] Support for cylindrical coordinate system |
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|`Mono(i)%loc(j)`| Real | $j$-th coordinate of the point that consists of $i$-th source plane |
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|`Mono(i)%dir`| Real | Direction of acoustic propagation |
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|`Mono(i)%mag`| Real | Pulse magnitude |
@@ -330,7 +330,7 @@ The $i$-th source plane is determined by the point at [`Mono(i)%loc(1)`, `Mono(i
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The source plane is defined in the finite region of the domain: $x\in[-\infty,\infty]$ and $y\in$[-`mymono_length`/2, `mymono_length`/2].\\
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`Mono(i)%support` $=3$ specifies a semi-infinite source plane in 3-D simulation.
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The $i$-th source plane is determined by the point at [`Mono(i)%loc(1)`, `Mono(i)%loc(2)`, `Mono(i)%loc(3)`] and the normal vector [$\mathrm{cos}$(`Mono(i)%dir`), $\mathrm{sin}$(`Mono(i)%dir`), 1] that consists of this point.
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The source plane is defined in the finite region of the domain: $x\in[-\infty,\infty]$ and $y,z\in$[-`mymono_length`/2, `mymono_length`/2]. There are a few additional spatial support types available for special source types and coordinate systems.
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The source plane is defined in the finite region of the domain: $x\in[-\infty,\infty]$ and $y,z\in$[-`mymono_length`/2, `mymono_length`/2]. There are a few additional spatial support types available for special source types and coordinate systems tabulated in [Monopole supports](#monopole-supports).
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