From bb6d3d41a1fab9c9363d1955fc899dfc884be6da Mon Sep 17 00:00:00 2001 From: Luke Labrie-Cleary Date: Wed, 9 Aug 2023 10:08:14 +0200 Subject: [PATCH] Update README.md --- dynamic_model/README.md | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/dynamic_model/README.md b/dynamic_model/README.md index d14b21f..f7613a1 100644 --- a/dynamic_model/README.md +++ b/dynamic_model/README.md @@ -52,7 +52,7 @@ The equations governing heat transfer contain three terms; a source term and a s ``` "Here, $W_f$ is the mass flow rate of fuel salt, $m_{f1}$ and $m_{f2}$ represent the mass of fuel nodes 1 and 2 respectively, $C_{pf}$ represents the fuel salt specific heat capacity, $K_1$ and $K_2$ are the fraction of total power generated in fuel nodes 1 and 2, $K_{g1}$ and $K_{g2}$ represent the fraction of power generated in the graphite transferred to each fuel node, $hA_{fg}$ is the product of area and heat transfer coefficient for the fuel-graphite interface, $P_0$ is the nominal power which multiplied with fractional neutron density n/no gives the instantaneous power, and the $T$s represent the temperatures of the various nodes. Note that the direction of heat transfer depends on the instantaneous temperature of the various nodes." (Singh et. al). -## Method +# Method The model herein uses SciPy's ODE library. Sample implementation is shown below: ```python