jupyter/m3c2.ipynb

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   "source": [
    "# Basic M3C2 algorithm"
   ]
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  {
   "cell_type": "markdown",
   "id": "1",
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   "source": [
    "This presents how the M3C2 algorithm ([Lague et al., 2013](#References)) for point cloud distance computation can be run using the `py4dgeo` package. As a first step, we import the `py4dgeo` and `numpy` packages:"
   ]
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   "source": [
    "import numpy as np\n",
    "import py4dgeo"
   ]
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   "source": [
    "Next, we need to load two datasets that cover the same scene at two different points in time. Point cloud datasets are represented by `numpy` arrays of shape `n x 3` using a 64 bit floating point type (`np.float64`). Here, we work with a rather small synthetical data set:"
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   "id": "4",
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   "outputs": [],
   "source": [
    "epoch1, epoch2 = py4dgeo.read_from_xyz(\n",
    "    \"plane_horizontal_t1.xyz\", \"plane_horizontal_t2.xyz\"\n",
    ")"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "5",
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   "source": [
    "The analysis of point cloud distances is executed on so-called *core points* (cf. Lague et al., 2013). These could be, e.g., one of the input point clouds, a subsampled version thereof, points in an equidistant grid, etc. Here, we choose a subsampling by taking every 50th point of the reference point cloud:"
   ]
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   "cell_type": "code",
   "execution_count": null,
   "id": "6",
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   "source": [
    "corepoints = epoch1.cloud[::50]"
   ]
  },
  {
   "cell_type": "markdown",
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   "source": [
    "Next, we instantiate the algorithm class and run the distance calculation:"
   ]
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   "source": [
    "m3c2 = py4dgeo.M3C2(\n",
    "    epochs=(epoch1, epoch2),\n",
    "    corepoints=corepoints,\n",
    "    cyl_radii=(2.0,),\n",
    "    normal_radii=(0.5, 1.0, 2.0),\n",
    ")\n",
    "\n",
    "distances, uncertainties = m3c2.run()"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "9",
   "metadata": {},
   "source": [
    "The calculated result is an array  with one distance per core point. The order of distances corresponds exactly to the order of input core points."
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "10",
   "metadata": {},
   "outputs": [],
   "source": [
    "distances"
   ]
  },
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   "cell_type": "markdown",
   "id": "11",
   "metadata": {},
   "source": [
    "Corresponding to the derived distances, an uncertainty array is returned which contains several quantities that can be accessed individually: The level of detection `lodetection`, the spread of the distance across points in either cloud (`spread1` and `spread2`, by default measured as the standard deviation of distances) and the total number of points taken into consideration in either cloud (`num_samples1` and `num_samples2`):"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "12",
   "metadata": {},
   "outputs": [],
   "source": [
    "uncertainties[\"lodetection\"]"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "13",
   "metadata": {},
   "outputs": [],
   "source": [
    "uncertainties[\"spread1\"]"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "14",
   "metadata": {},
   "outputs": [],
   "source": [
    "uncertainties[\"num_samples1\"]"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "15",
   "metadata": {},
   "source": [
    "### References\n",
    "\n",
    "* Lague, D., Brodu, N., & Leroux, J. (2013). Accurate 3D comparison of complex topography with terrestrial laser scanner: Application to the Rangitikei canyon (N-Z). ISPRS Journal of Photogrammetry and Remote Sensing, 82, pp. 10-26. doi: [10.1016/j.isprsjprs.2013.04.009](https://doi.org/10.1016/j.isprsjprs.2013.04.009)."
   ]
  }
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