Linear¤
exponax.stepper.generic.DifficultyLinearStepper
¤
Bases: NormalizedLinearStepper
Source code in exponax/stepper/generic/_linear.py
234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 |
|
__init__
¤
__init__(
num_spatial_dims: int = 1,
num_points: int = 48,
*,
linear_difficulties: tuple[float, ...] = (0.0, -2.0)
)
Timestepper for d-dimensional (d ∈ {1, 2, 3}
) linear PDEs on periodic
boundary conditions with normalized dynamics in a difficulty-based
interface.
Different to NormalizedLinearStepper
, the dynamics are defined by
difficulties. The difficulties are a different combination of normalized
dynamics, num_spatial_dims
, and num_points
.
γᵢ = αᵢ Nⁱ 2ⁱ⁻¹ d
with d
the number of spatial dimensions, N
the number of points, and
αᵢ
the normalized coefficient.
This interface is more natural because the difficulties for all orders
(given by i
) are around 1.0. Additionally, they relate to stability
condition of explicit Finite Difference schemes for the particular
equations. For example, for advection (i=1
), the absolute of the
difficulty is the Courant-Friedrichs-Lewy (CFL) number.
In the default configuration of this timestepper, the PDE is an advection equation with CFL number 2 solved in 1d with 48 resolution points to discretize the domain.
Arguments:
num_spatial_dims
: The number of spatial dimensionsd
. Default is 1.num_points
: The number of pointsN
used to discretize the domain. This includes the left boundary point and excludes the right boundary point. In higher dimensions; the number of points in each dimension is the same. Hence, the total number of degrees of freedom isNᵈ
. Default is 48.difficulties
: The difficulties of the normalized dynamics. This must be a tuple of floats. The length of the tuple defines the highest occuring linear derivative in the PDE. Default is(0.0, -2.0)
.
Source code in exponax/stepper/generic/_linear.py
237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 |
|
__call__
¤
__call__(
u: Float[Array, "C ... N"]
) -> Float[Array, "C ... N"]
Perform one step of the time integration for a single state.
Arguments:
u
: The state vector, shape(C, ..., N,)
.
Returns:
u_next
: The state vector after one step, shape(C, ..., N,)
.
Tip
Use this call method together with exponax.rollout
to efficiently
produce temporal trajectories.
Info
For batched operation, use jax.vmap
on this function.
Source code in exponax/_base_stepper.py
240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 |
|