Background:
I am doing experiments trying to map the practical solubility of a certain chemical species called an "activator" solution. This solution is essentially a sequential mixture of water, $NaOH$ pellets and aqueous sodium silicate. In short (without getting into too much background), my results will help me determine if I can use certain chemical species in some very environmentally friendly materials science applications.
One of the parameters to keep track of is the temperature of solution which changes the solubility of the activator. I need to model this as I've found identical solutions respond differently when the final sodium silicate ingredient is added to the aqueous $NaOH$ solution at different temperatures. Here is some experimental data from the lab showing T vs t:
Essentially, there are 2 main "periods" during the experiment:
- The Initial Temperature Rise (i.e. from $T_i$ = 23.4 $^{\circ} C$ = ambient temperature $\rightarrow$ $T_{Max}$ = 97 $^{\circ} C$).
- The Cooldown Period (i.e. from $T_{Max} \rightarrow T_i$)
Here is a picture of the experimental setup showing 2 x ~200mL of activator in a conical flask. Both activators were made the same initially but on the left, the sodium silicate was added at ambient temperatures (which caused precipitation) as opposed to the right, where the sodium silicate was added at around 80% of $T_{Max}$.
Problem:
I'm wanting to model the T vs t for the system (similar to the experimental data above) so I can see the temperature profile of different activators with different chemical ratios. It seems, fundamentally, to start with an energy balance with:
$$\frac{dQ}{dt} = Q_{in} - Q_{out} + Q_{rxn}$$
Assuming no heat input, a known value for $Q_{rxn}$ (from a previous question of mine) and $Q_{out} = Q_{Conduction,Plate} + Q_{Convection,surroundings}$ I'm wondering the following:
- How should the system be modelled? is it good to model $Q_{out}$ with the heat equation and solve for T (as per pic below)? On that, how do I even solve for t? I have minimal knowledge of Fourier transforms.