4. stars data model

For a better version of the stars vignettes see https://r-spatial.github.io/stars/articles/

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This vignette explains the data model of stars objects, illustrated using artificial and real datasets.

Stars objects

stars objects consist of

A dimensions object is a named list of dimension elements, each describing the semantics a dimension of the data arrays (space, time, type etc). In addition to that, a dimensions object has an attribute called raster of class stars_raster, which is a named list with three elements:

The affine and curvilinear values are only relevant in case of raster data, indicated by dimensions to have non-NA values.

A dimension object describes a single dimension; it is a list with named elements

from and to will usually be 1 and the dimension size, but from may be larger than 1 in case a sub-grid got was selected (or cropped).

offset and delta only apply to regularly discretized dimensions, and are NA if this is not the case. If they are NA, dimension values may be held in the values field. Rectilinear and curvilinear grids need grid values in values that can be either:

Alternatively, values can contains a set of spatial geometries encoded in an sfc vector ("list-column"), in which case we have a vector data cube.

Grid type

Regular grids

With a very simple file created from a $4 \times 5$ matrix

suppressPackageStartupMessages(library(stars))
m = matrix(1:20, nrow = 5, ncol = 4)
dim(m) = c(x = 5, y = 4) # named dim
(s = st_as_stars(m))

we see that

dim(s[[1]])

When we plot this object, using the image method for stars objects,

image(s, text_values = TRUE, axes = TRUE)

we see that $(0,0)$ is the origin of the grid (grid corner), and $1$ the coordinate value increase from one index (row, col) to the next. It means that consecutive matrix columns represent grid lines, going from south to north. Grids defined this way are regular: grid cell size is constant everywhere.

Many actual grid datasets have y coordinates (grid rows) going from North to South (top to bottom); this is realised with a negative value for delta. We see that the grid origing $(0,0)$ did not change:

attr(s, "dimensions")[[2]]$delta = -1
image(s, text_values = TRUE, axes = TRUE)

An example is the GeoTIFF carried in the package, which, as probably all data sources read through GDAL, has a negative delta for the y-coordinate:

tif = system.file("tif/L7_ETMs.tif", package = "stars")
st_dimensions(read_stars(tif))["y"]

Raster attributes, rotated and sheared grids

Dimension tables of stars objects carry a raster attribute:

str(attr(st_dimensions(s), "raster"))

which is a list that holds

These fields are needed at this level, because they describe properties of the array at a higher level than individual dimensions do: a pair of dimensions forms a raster, both affine and curvilinear describe how x and y as a pair are derived from grid indexes (see below) when this cannot be done on a per-dimension basis.

With two affine parameters $a_1$ and $a_2$, $x$ and $y$ coordinates are derived from (1-based) grid indexes $i$ and $j$, grid offset values $o_x$ and $o_y$, and grid cell sizes $d_x$ and $d_y$ by

$$x = o_x + (i-1) d_x + (j-1) a_1$$

$$y = o_y + (i-1) a_2 + (j-1) d_y$$ Clearly, when $a_1=a_2=0$, $x$ and $y$ are entirely derived from their respective index, offset and cellsize.

Note that for integer indexes, the coordinates are that of the starting edge of a grid cell; to get the grid cell center of the top left grid cell (in case of a negative $d_y$), use $i=1.5$ and $j=1.5$.

We can rotate grids by setting $a_1$ and $a_2$ to a non-zero value:

attr(attr(s, "dimensions"), "raster")$affine = c(0.1, 0.1)
plot(st_as_sf(s, as_points = FALSE), axes = TRUE, nbreaks = 20)

The rotation angle, in degrees, is

atan2(0.1, 1) * 180 / pi

Sheared grids are obtained when the two rotation coefficients, $a_1$ and $a_2$, are unequal:

attr(attr(s, "dimensions"), "raster")$affine = c(0.1, 0.2)
plot(st_as_sf(s, as_points = FALSE), axes = TRUE, nbreaks = 20)

Now, the y-axis and x-axis have different rotation in degrees of respectively

atan2(c(0.1, 0.2), 1) * 180 / pi

Rectilinear grids

Rectilinear grids have orthogonal axes, but do not have congruent (equally sized and shaped) cells: each axis has its own irregular subdivision.

We can define a rectilinear grid by specifying the cell boundaries, meaning for every dimension we specify one more value than the dimension size:

x = c(0, 0.5, 1, 2, 4, 5)  # 6 numbers: boundaries!
y = c(0.3, 0.5, 1, 2, 2.2) # 5 numbers: boundaries!
(r = st_as_stars(list(m = m), dimensions = st_dimensions(x = x, y = y)))
st_bbox(r)
image(r, axes = TRUE, col = grey((1:20)/20))

Would we leave out the last value, than stars may come up with a different cell boundary for the last cell, as this is now derived from the width of the one-but-last cell:

x = c(0, 0.5, 1, 2, 4)  # 5 numbers: offsets only!
y = c(0.3, 0.5, 1, 2)   # 4 numbers: offsets only!
(r = st_as_stars(list(m = m), dimensions = st_dimensions(x = x, y = y)))
st_bbox(r)

This is not problematic if cells have a constant width, in which case the boundaries are reduced to an offset and delta value, irrespective whether an upper boundary is given:

x = c(0, 1, 2, 3, 4)  # 5 numbers: offsets only!
y = c(0.5, 1, 1.5, 2)   # 4 numbers: offsets only!
(r = st_as_stars(list(m = m), dimensions = st_dimensions(x = x, y = y)))
st_bbox(r)

Alternatively, one can also set the cell midpoints by specifying arguments cell_midpoints to the st_dimensions call:

x = st_as_stars(matrix(1:9, 3, 3), 
                st_dimensions(x = c(1, 2, 3), y = c(2, 3, 10), cell_midpoints = TRUE))

When the dimension is regular, this results in offset being shifted back with half a delta, or else in intervals derived from the distances between cell centers. This should obviously not be done when cell boundaries are specified.

Curvilinear grids

Curvilinear grids are grids whose grid lines are not straight. Rather than describing the curvature parametrically, the typical (HDF5 or NetCDF) files in which they are found have two raster layers with the longitudes and latitudes for every corresponding pixel of remaining layers.

As an example, we will use a Sentinel 5P dataset available from package starsdata; this package can be installed with

install.packages("starsdata", repos = "http://pebesma.staff.ifgi.de", type = "source") 

The dataset is found here:

(s5p = system.file("sentinel5p/S5P_NRTI_L2__NO2____20180717T120113_20180717T120613_03932_01_010002_20180717T125231.nc", package = "starsdata"))
EVAL = s5p != ""

We can construct the curvilinear stars raster by calling read_stars on the right sub-array:

subs = gdal_subdatasets(s5p)
subs[[6]]

For this array, we can see the GDAL metadata under item GEOLOCATION:

gdal_metadata(subs[[6]], "GEOLOCATION")

which reveals where, in this dataset, the longitude and latitude arrays are kept.

nit.c = read_stars(subs[[6]]) 
threshold = units::set_units(9e+36, mol/m^2)
nit.c[[1]][nit.c[[1]] > threshold] = NA
nit.c

The curvilinear array has the actual arrays (raster layers, matrices) with longitude and latitude values read in its dimension table. We can plot this file:

plot(nit.c, breaks = "equal", reset = FALSE, axes = TRUE, as_points = TRUE, 
         pch = 16,  logz = TRUE, key.length = 1)
maps::map('world', add = TRUE, col = 'red')
plot(nit.c, breaks = "equal", reset = FALSE, axes = TRUE, as_points = FALSE, 
         border = NA, logz = TRUE, key.length = 1)
maps::map('world', add = TRUE, col = 'red')

We can downsample the data by

(nit.c_ds = stars:::st_downsample(nit.c, 8))
plot(nit.c_ds, breaks = "equal", reset = FALSE, axes = TRUE, as_points = TRUE, 
         pch = 16, logz = TRUE, key.length = 1)
maps::map('world', add = TRUE, col = 'red')

which doesn't look nice, but plotting the cells as polygons looks better:

plot(nit.c_ds, breaks = "equal", reset = FALSE, axes = TRUE, as_points = FALSE, 
         border = NA, logz = TRUE, key.length = 1)
maps::map('world', add = TRUE, col = 'red')

Another approach would be to warp the curvilinear grid to a regular grid, e.g. by

w = st_warp(nit.c, crs = 4326, cellsize = 0.25)
plot(w)


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stars documentation built on Sept. 11, 2023, 5:10 p.m.