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*Last updated: 2023-03-16.*

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# tf_quant_finance.math.pde.fd_solvers.solve_forward

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<a target="_blank" href="https://github.com/paolodelia99/tf-quant-finance/blob/main/tf_quant_finance/math/pde/fd_solvers.py">View source</a>



Evolves a grid of function values forward in time according to a PDE.

```python
tf_quant_finance.math.pde.fd_solvers.solve_forward(
    start_time, end_time, coord_grid, values_grid, num_steps=None,
    start_step_count=0, time_step=None, one_step_fn=None, boundary_conditions=None,
    values_transform_fn=None, second_order_coeff_fn=None, first_order_coeff_fn=None,
    zeroth_order_coeff_fn=None, inner_second_order_coeff_fn=None,
    inner_first_order_coeff_fn=None, maximum_steps=None, swap_memory=True,
    dtype=None, name=None
)
```



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Evolves a discretized solution of following second order linear
partial differential equation:

```None
  dV/dt + Sum[a_ij d2(A_ij V)/dx_i dx_j, 1 <= i, j <=n] +
     Sum[b_i d(B_i V)/dx_i, 1 <= i <= n] + c V = 0.
```
from time `t0` to time `t1 > t0` (i.e. forward in time). Here `a_ij`,
`A_ij`, `b_i`, `B_i` and `c` are coefficients that may depend on spatial
variables `x` and time `t`.

See more details in `solve_backwards()`: other than the forward time
direction, the specification is the same.

#### Args:


* <b>`start_time`</b>: Real scalar `Tensor`. The start time of the grid.
  Corresponds to time `t0` above.
* <b>`end_time`</b>: Real scalar `Tensor` larger than the `start_time`.
   The time to evolve forward to. Corresponds to time `t1` above.
* <b>`coord_grid`</b>: List of `n` rank 1 real `Tensor`s. `n` is the dimension of the
  domain. The i-th `Tensor` has shape either `[d_i]` or ` B + [d_i]` where
  `d_i` is the size of the grid along axis `i` and `B` is a batch shape. The
  coordinates of the grid points. Corresponds to the spatial grid `G` above.
* <b>`values_grid`</b>: Real `Tensor` containing the function values at time
  `start_time` which have to be evolved to time `end_time`. The shape of the
  `Tensor` must broadcast with `B + [d_1, d_2, ..., d_n]`. `b` is the batch
  dimensions (one or more), which allow multiple functions (with potentially
  different boundary/final conditions and PDE coefficients) to be evolved
  simultaneously.
* <b>`num_steps`</b>: Positive int scalar `Tensor`. The number of time steps to take
  when moving from `start_time` to `end_time`. Either this argument or the
  `time_step` argument must be supplied (but not both). If num steps is
  `k>=1`, uniform time steps of size `(t1 - t0)/k` are taken to evolve the
  solution from `t0` to `t1`. Corresponds to the `n_steps` parameter above.
* <b>`start_step_count`</b>: A scalar integer `Tensor`. Number of steps performed so
  far.
* <b>`time_step`</b>: The time step to take. Either this argument or the `num_steps`
  argument must be supplied (but not both). The type of this argument may
  be one of the following (in order of generality):
    (a) None in which case `num_steps` must be supplied.
    (b) A positive real scalar `Tensor`. The maximum time step to take.
      If the value of this argument is `dt`, then the total number of steps
      taken is N = (t1 - t0) / dt rounded up to the nearest integer. The
      first N-1 steps are of size dt and the last step is of size
      `t1 - t0 - (N-1) * dt`.
    (c) A callable accepting the current time and returning the size of the
      step to take. The input and the output are real scalar `Tensor`s.
* <b>`one_step_fn`</b>: The transition kernel. A callable that consumes the following
  arguments by keyword:
    1. 'time': Current time
    2. 'next_time': The next time to step to. For the backwards in time
      evolution, this time will be smaller than the current time.
    3. 'coord_grid': The coordinate grid.
    4. 'values_grid': The values grid.
    5. 'second_order_coeff_fn': Callable returning the coefficients of the
      second order terms of the PDE. See the spec of the
      `second_order_coeff_fn` argument below.
    6. 'first_order_coeff_fn': Callable returning the coefficients of the
      first order terms of the PDE. See the spec of the
      `first_order_coeff_fn` argument below.
    7. 'zeroth_order_coeff_fn': Callable returning the coefficient of the
      zeroth order term of the PDE. See the spec of the
      `zeroth_order_coeff_fn` argument below.
    8. 'num_steps_performed': A scalar integer `Tensor`. Number of steps
      performed so far.
   The callable should return a sequence of two `Tensor`s. The first one
   is a `Tensor` of the same `dtype` and `shape` as `coord_grid` and
   represents a new coordinate grid after one iteration. The second `Tensor`
   is of the same shape and `dtype` as`values_grid` and represents an
   approximate solution of the equation after one iteration.
   Default value: None, which means Crank-Nicolson scheme with oscillation
   damping is used for 1D problems, and Douglas ADI scheme with `theta=0.5`
   - for multidimensional problems.
* <b>`boundary_conditions`</b>: The boundary conditions. Only rectangular boundary
  conditions are supported. A list of tuples of size `n` (space dimension
  of the PDE). The elements of the Tuple can be either a Python Callable or
  `None` representing the boundary conditions at the minimum and maximum
  values of the spatial variable indexed by the position in the list. E.g.,
  for `n=2`, the length of `boundary_conditions` should be 2,
  `boundary_conditions[0][0]` describes the boundary `(y_min, x)`, and
  `boundary_conditions[1][0]`- the boundary `(y, x_min)`. `None` values mean
  that the second order terms for that dimension on the boundary are assumed
  to be zero, i.e., if `boundary_conditions[k][0]` is None,
  'dV/dt + Sum[a_ij d2(A_ij V)/dx_i dx_j, 1 <= i, j <=n, i!=k+1, j!=k+1] +
     Sum[b_i d(B_i V)/dx_i, 1 <= i <= n] + c V = 0.'
  For not `None` values, the boundary conditions are accepted in the form
  `alpha(t, x) V + beta(t, x) V_n = gamma(t, x)`, where `V_n` is the
  derivative with respect to the exterior normal to the boundary.
  Each callable receives the current time `t` and the `coord_grid` at the
  current time, and should return a tuple of `alpha`, `beta`, and `gamma`.
  Each can be a number, a zero-rank `Tensor` or a `Tensor` whose shape is
  the grid shape with the corresponding dimension removed.
  For example, for a two-dimensional grid of shape `(b, ny, nx)`, where `b`
  is the batch size, `boundary_conditions[0][i]` with `i = 0, 1` should
  return a tuple of either numbers, zero-rank tensors or tensors of shape
  `(b, nx)`. Similarly for `boundary_conditions[1][i]`, except the tensor
  shape should be `(b, ny)`. `alpha` and `beta` can also be `None` in case
  of Neumann and Dirichlet conditions, respectively.
  Default value: `None`. Unlike setting `None` to individual elements of
  `boundary_conditions`, setting the entire `boundary_conditions` object to
  `None` means Dirichlet conditions with zero value on all boundaries are
  applied.
* <b>`values_transform_fn`</b>: An optional callable applied to transform the solution
  values at each time step. The callable is invoked after the time step has
  been performed. The callable should accept the time of the grid, the
  coordinate grid and the values grid and should return the values grid. All
  input arguments to be passed by keyword.
  It returns the updated value grid and the coordinate grid, which may be
  updated as well.
* <b>`second_order_coeff_fn`</b>: Callable returning the coefficients of the second
  order terms of the PDE (i.e. `a_{ij}(t, x)` above) at given time `t`.
  The callable accepts the following arguments:
    `t`: The time at which the coefficient should be evaluated.
    `coord_grid`: a `Tensor` representing a grid of locations `r` at which
      the coefficient should be evaluated.
  Returns the object `a` such that `a[i][j]` is defined and
  `a[i][j]=a_{ij}(r, t)`, where `0 <= i < n_dims` and `i <= j < n_dims`.
  For example, the object may be a list of lists or a rank 2 Tensor.
  `a[i][j]` is assumed to be symmetrical, and only the elements with
  `j >= i` will be used, so elements with `j < i` can be `None`.
  Each `a[i][j]` should be a Number, a `Tensor` broadcastable to the shape
  of `coord_grid`, or `None` if corresponding term is absent in the
  equation. Also, the callable itself may be None, meaning there are no
  second-order derivatives in the equation.
  For example, for a 2D equation with the following second order terms
  ```
  a_xx V_xx + 2 a_xy V_xy + a_yy V_yy
  ```
   the callable may return either
  `[[a_yy, a_xy], [a_xy, a_xx]]` or `[[a_yy, a_xy], [None, a_xx]]`.
  Default value: None. If both `second_order_coeff_fn` and
    `inner_second_order_coeff_fn` are None, it means the second-order term
    is absent. If only one of them is `None`, it is assumed to be `1`.
* <b>`first_order_coeff_fn`</b>: Callable returning the coefficients of the
  first order terms of the PDE (i.e. `mu_i(t, r)` above) evaluated at given
  time `t`.
  The callable accepts the following arguments:
    `t`: The time at which the coefficient should be evaluated.
    `locations_grid`: a `Tensor` representing a grid of locations `r` at
      which the coefficient should be evaluated.
  Returns a list or an 1D `Tensor`, `i`-th element of which represents
  `b_i(t, r)`. Each element is a `Tensor` broadcastable to the shape of
  `locations_grid`, or None if corresponding term is absent in the
  equation. The callable itself may be None, meaning there are no
  first-order derivatives in the equation.
  Default value: None. If both `first_order_coeff_fn` and
    `inner_first_order_coeff_fn` are None, it means the first-order term is
    absent. If only one of them is `None`, it is assumed to be `1`.
* <b>`zeroth_order_coeff_fn`</b>: Callable returning the coefficient of the
  zeroth order term of the PDE (i.e. `c(t, r)` above) evaluated at given
  time `t`.
  The callable accepts the following arguments:
    `t`: The time at which the coefficient should be evaluated.
    `locations_grid`: a `Tensor` representing a grid of locations `r` at
      which the coefficient should be evaluated.
  Should return a `Tensor` broadcastable to the shape of `locations_grid`.
  May return None or be None if the shift term is absent in the equation.
  Default value: None, meaning absent zeroth order term.
* <b>`inner_second_order_coeff_fn`</b>: Callable returning the coefficients under the
  second derivatives (i.e. `A_ij(t, x)` above) at given time `t`. The
  requirements are the same as for `second_order_coeff_fn`.
* <b>`inner_first_order_coeff_fn`</b>: Callable returning the coefficients under the
  first derivatives (i.e. `B_i(t, x)` above) at given time `t`. The
  requirements are the same as for `first_order_coeff_fn`.
* <b>`maximum_steps`</b>: Optional int `Tensor`. The maximum number of time steps that
  might be taken. This argument is only used if the `num_steps` is not used
  and `time_step` is a callable otherwise it is ignored. It is useful to
  supply this argument to ensure that the time stepping loop can be
  optimized. If the argument is supplied and used, the time loop with
  execute at most these many steps so it is important to ensure that this
  parameter is an upper bound on the number of expected steps.
* <b>`swap_memory`</b>: Whether GPU-CPU memory swap is enabled for this op. See
  equivalent flag in `tf.while_loop` documentation for more details. Useful
  when computing a gradient of the op.
* <b>`dtype`</b>: The dtype to use.
  Default value: None, which means dtype will be inferred from
  `values_grid`.
* <b>`name`</b>: The name to give to the ops.
  Default value: None which means `solve_forward` is used.


#### Returns:

The final values grid, final coordinate grid, final time and number of steps
performed.



#### Raises:

ValueError if neither num steps nor time steps are provided or if both
are provided.
