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authorAnton Khirnov <anton@khirnov.net>2014-11-01 15:00:30 +0100
committerAnton Khirnov <anton@khirnov.net>2014-11-01 15:00:30 +0100
commite421ae2d7df9bd6bae9e45e33fe76f31a8229a53 (patch)
treeba2d79eccc1c55fbd3d9e7f967a75f9ef8ec75c6 /brill_data.h
parent24499694116ff25a190e95533da09d0efaccffae (diff)
Add a function for evaluating ψ.
Diffstat (limited to 'brill_data.h')
-rw-r--r--brill_data.h23
1 files changed, 23 insertions, 0 deletions
diff --git a/brill_data.h b/brill_data.h
index b8b63e8..85e1aac 100644
--- a/brill_data.h
+++ b/brill_data.h
@@ -138,3 +138,26 @@ void bd_context_free(BDContext **bd);
* @return >= 0 on success, a negative error code on failure
*/
int bd_solve(BDContext *bd);
+
+/**
+ * Evaluate the conformal factor ψ or its derivatives at the specified rectangular grid.
+ *
+ * @param bd the solver context
+ * @param rho the array of ρ coordinates.
+ * @param nb_coords_rho the number of elements in rho.
+ * @param z the array of z coordinates.
+ * @param nb_coords_z the number of elements in z.
+ * @param diff_order the order of the derivatives of ψ to evaluate. The first element specifies the
+ * derivative wrt ρ, the second wrt z. I.e. diff_order = { 0, 0 } evaluates ψ
+ * itself, diff_order = { 0, 1 } evaluates ∂ψ/∂z etc.
+ * @param psi the array into which the values of ψ will be written. ψ is evaluated on the grid
+ * formed by the outer product of the rho and z vectors.
+ * I.e. psi[j * nb_coords_rho + i] = ψ(rho[i], z[j]). The length of psi must be
+ * nb_coords_rho * nb_coords_z.
+ *
+ * @return >= 0 on success, a negative error code on failure.
+ */
+int bd_eval_psi(BDContext *bd, const double *rho, int nb_coords_rho,
+ const double *z, int nb_coords_z,
+ const unsigned int diff_order[2],
+ double *psi);