* The pressure is given by * \f{align} * p = (\gamma - 1) \rho e * \f} */

* The pressure is given by * \f{align} * p = (\gamma - 1) * (\rho * e + a \rho^2)/(1 - b \rho) - a \rho^2 * \f} */

* The pressure is given by * \f{align} * p = (\gamma - 1) \rho (e - q) / (1 - b \rho) - \gamma p_\infty * \f} */

* The pressure is given by * \f{align} * p = 0.0 * \f} */

* Variant of above function operating on a contiguous range of * values. The result is stored in the first argument @p p, * overriding p

* The pressure is given by * \f{align} * p = A(1 - \omega / R_1 \rho / \rho_0) e^{(-R_1 \rho_0 / \rho)} * + B(1 - \omega /

* The pressure is given by the formula (19) in reference. */

* Print a status line with solver statistics. This function is used * for constructing the status message displayed periodically in the * Ti

* Given a state @p U_i and an index @p i return "strict" bounds, * i.e., a minimal convex set containing the state. */

* Reinit with a scalar partitioner */

* (Re)initialize the parabolic state vector component of the state * vector. * * @note This routine does not modify the hyperbolic stat

* (Re)initialize the parabolic state vector component of the state * vector. * * @note This routine does not modify the hyperboli

* Reset temporary storage */

* Reset temporary storage and initialize for a new row corresponding * to state vector U_i. */

* Sets the invariant domain violation strategy. */

* Sets the invariant domain violation strategy. */

* The specific internal energy is given by * \f{align} * e = p / (\rho (\gamma - 1)) * \f} */

* The specific internal energy is given by * \f{align} * \rho e = (p + a \rho^2) * (1 - b \rho) / (\rho (\gamma -1)) * - a \r

* The specific internal energy is given by * \f{align} * e - q = (p + \gamma p_\infty) * (1 - b \rho) / (\rho (\gamma - 1)) * \

* The specific internal energy is given by * \f{align} * e = 0 * \f} */

* Variant of above function operating on a contiguous range of * values. The result is stored in the first argument @p p, * overriding p

* The specific internal energy is given by * \f{align} * \omega \rho e = p * - A(1 - \omega / R_1 \rho / \rho_0) e^{(-R_1 \rh

* The specific internal energy is given by a complicated formula. */

* The speed of sound is given by * \f{align} * c^2 = \gamma * (\gamma - 1) e * \f} */

* The speed of sound is given by * \f{align} * c^2 = \frac{\gamma (\gamma -1) (e + a \rho)}{(1 - b\rho)^2} * - 2a\rho.

* Let \f$X = (1 - b \rho)\f$. The speed of sound is given by * \f{align} * c^2 = \frac{\gamma (p + p_\infty)}{\rho X} * =

* The speed of sound is given by * \f{align} * c^2 = 0 * \f} */

* Variant of above function operating on a contiguous range of * values. The result is stored in the first argument @p p, * overriding p

* The speed of sound is given by */

* The speed of sound is given by equation (21) in reference. */