diff --git a/docs/source/input.rst b/docs/source/input.rst index 2cd6cad7..1aeb11d1 100644 --- a/docs/source/input.rst +++ b/docs/source/input.rst @@ -38,9 +38,9 @@ The commands have been grouped into six categories: * **Essential** - required to run any model, such as the domain size and spatial discretization * **General** - provide further control over the model -* **Media** - used to introduce different materials into the model +* **Material** - used to introduce different materials into the model * **Object construction** - used to build geometric shapes with different constitutive parameters -* **Excitation and output** - used to place source and output points in the model +* **Source and output** - used to place source and output points in the model * **PML** - provide advanced customisation and optimisation of the absorbing boundary conditions Essential commands @@ -221,8 +221,8 @@ For example to save a snapshot of the electromagnetic fields in the model at a s .. _materials: -Media commands -============== +Material commands +================= Built-in materials ------------------ @@ -623,8 +623,8 @@ For example, to apply 100 blades of grass that vary in height between 100 and 15 * The grass is modelled using a single-pole Debye formulation with properties :math:`\epsilon_{rs} = 18.5087`, :math:`\epsilon_{\infty} = 12.7174`, and a relaxation time of :math:`\tau = 1.0793 \times 10^{-11}` seconds (http://dx.doi.org/10.1007/BF00902994). If you prefer, gprMax will use your own definition for grass if you use a material named ``grass``. The geometry of the blades of grass are defined by the parametric equations: :math:`x = x_c +s_x {\left( \frac{t}{b_x} \right)}^2`, :math:`y = y_c +s_y {\left( \frac{t}{b_y} \right)}^2`, and :math:`z=t`, where :math:`s_x` and :math:`s_y` can be -1 or 1 which are randomly chosen, and where the constants :math:`b_x` and :math:`b_y` are random numbers based on a Gaussian distribution. -Excitation commands -=================== +Source and output commands +========================== #waveform: ----------