diff options
| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 15:46:52 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 15:46:52 +0100 |
| commit | 20ffb069058bca966cdae3f9648d22aead958728 (patch) | |
| tree | 439568be95b0c652e029912ee3118489b6c40ded /typst | |
| parent | d8640dc3c4f971d577a27c0f848892a1657f112c (diff) | |
| download | phd-fluid_mechanics_report-20ffb069058bca966cdae3f9648d22aead958728.tar.gz | |
progress
Diffstat (limited to 'typst')
| -rw-r--r-- | typst/main.typ | 5 |
1 files changed, 3 insertions, 2 deletions
diff --git a/typst/main.typ b/typst/main.typ index e47c56c..6b64e01 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -192,14 +192,15 @@ The mass balance equation for the fluid phase then reads #math.equation( block:true, $ -delta (epsilon rho_f) / (delta t) + nabla ( epsilon rho_f v^f) = 0 +partial (epsilon rho_f) / (partial t) + nabla ( epsilon rho_f v^f) = 0 $ ) with a fluid momentum balance equation #math.equation( block:true, -$ delta(epsilon rho_f v^f) / (delta t) + nabla (epsilon rho_f v^f v^f ) = - epsilon rho_f g + epsilon nabla\ +$ +partial(epsilon rho_f v^f) / (partial t) + nabla (epsilon rho_f v^f v^f ) = - epsilon rho_f g + epsilon nabla\ (mu_f (nabla v^f + (nabla v^f)^T) - epsilon^2 mu_f ( v^f - v^p) / K). $ ) |