Lab Notebook Entry #15

46 hours/10 cycles into argon Zn-I test. New current collectors arrived!
lab notebook
research
flow batteries
doi
Author

Kirk Pollard Smith

Published

April 18, 2026

The test I started on April 16th continues. There is a leak from one of the barbed fittings, but three out of the four Luer Lock fittings are completely solid with no leaks, so I’d call their design a success, I probably just didn’t screw the leaky fitting in enough.

Iodine/triiodide visible near where the pinhole from the argon tubing is in the left (positive) reservoir septa, so methinks oxygen is sneaking in here still. Daniel suggested to add parafilm over it.

Yup that’s iodine leakage on the positive reservoir, from the fitting returning electrolyte to the reservoir.

Even after adding the parafilm, there was still more brown color on the positive reservoir septa (or maybe on top of the septa between the septa and the parafilm).

New current collectors arrived, these should allow for the kit to take up less space which will help fitting it into secondary containment

This is also the first test with argon sparging before cycling. Already the cycling behavior is different, it jumped straight to the 1.3 V charging plateau without any visible intermediate reactions. Also, there was strange non-monotonic behavior on the initial discharge cycles, which we have seen before and may be attributable to (iodine-containing) film formation. Perhaps things weren’t fully mixed before and it took time for the triethylene glycol to complex? In any case, it went away, so perhaps it was some sort of formation process.

I lost a few drops of electrolyte pulling the argon tubing out before the test, and like I mentioned, there is a small leak, so that definitely will affect the results, but here they are anyway. And here is ze data.

It’s been running for 46 hours now and has completed 10 cycles. Not going to comment on things as it’s still running. But the cell performance is actually improving with cycling! First couple cycles were weird.

Electrolyte Composition (molarity, per L solution) 0.92 M ZnCl2, 1.80 M NH4Cl, 0.76 M KI, 0.33 M triethylene glycol, 42.89 M H2O
Electrolyte Composition (molality, per kg solution) 0.74 m ZnCl2, 1.44 m NH4Cl, 0.60 m KI, 0.27 m triethylene glycol, 34.31 m H2O
Electrolyte Volume 5.5 mL (anolyte) + 5.5 mL (catholyte)
Electrolyte Density 1.3 g/mL
RFB Dev Kit commit e655c88f06
Cell Geometric Area 2 cm2
Separator Daramic AA-900
Anode Configuration Grafoil + 3.2 mm graphite felt
Cathode Configuration Grafoil + 3.2 mm graphite felt
Gaskets Outer and inner, 0.40 mm silicone (measured with micrometer)
Current Density 20 mA/cm2
Charging Conditions To 100 mAh (about 9 Ah/L) or 1.7 V
Discharging Conditions To 0 V
Flow Conditions Kamoer KPK200 24 V brushless peristaltic pumps at 40% duty cycle (about 1500 rpm) with 3x5 mm Tygon Chemical (PTFE-lined BPT) tubing, double reservoirs with Luer Lock barbed fittings
Inert Gas Sparged electrolyte through septa with argon for 15 minutes prior to cycling with pumps on
Code
import pandas as pd
from tqdm import tqdm, notebook
import numpy as np
import scipy
import plotly.express as px
import plotly.graph_objects as go
from plotly.subplots import make_subplots
import kaleido
from IPython.display import Image

tqdm_disabled = True  # True for website, change to False for local work

sampling = True

MIN_POINTS0 = 500
DIFF_LIMIT = 0.1


# electrolyte component masses, in g
MASS_ZnCl2  = 1.38
MASS_NH4Cl  = 1.06
MASS_KI     = 3.32
MASS_H2O    = 8.50
MASS_TriEG  = 0.55

total_mass_kg = (MASS_ZnCl2 + MASS_KI + MASS_H2O + MASS_TriEG) / 1000.0

TOTAL_VOLUME = 11  # electrolyte volume in mL, approx, measured by taking as much electrolyte as possible up into a 12 mL syringe

MASS_TO_RESERVOIRS = 14.60  # g of electrolyte actually loaded into system, based on weighing syringe before/after loading reservoirs
# molecular weights in g/mol

density = MASS_TO_RESERVOIRS / TOTAL_VOLUME

MW_ZnCl2 = 136.315
MW_NH4Cl = 53.49
MW_KI = 166.0028
MW_H2O = 18.01528
MW_TriEG = 150.174

molality_ZnCl2 = MASS_ZnCl2 / MW_ZnCl2 / total_mass_kg
molality_NH4Cl = MASS_NH4Cl / MW_NH4Cl / total_mass_kg
molality_KI = MASS_ZnCl2 / MW_KI / total_mass_kg
molality_TriEG = MASS_TriEG / MW_TriEG / total_mass_kg
molality_H2O = MASS_H2O / MW_H2O / total_mass_kg

molarity_ZnCl2 = MASS_ZnCl2 / MW_ZnCl2 / TOTAL_VOLUME * 1000.0
molarity_NH4Cl = MASS_NH4Cl / MW_NH4Cl / TOTAL_VOLUME * 1000.0
molarity_KI = MASS_ZnCl2 / MW_KI / TOTAL_VOLUME * 1000.0
molarity_TriEG = MASS_TriEG / MW_TriEG / TOTAL_VOLUME * 1000.0
molarity_H2O = MASS_H2O / MW_H2O / TOTAL_VOLUME * 1000.0


filenames = [
    "16-04-2026-KPS-22.zip",
]


all_data = []
for f in filenames:
    if len(all_data) == 0:
        all_data.append(pd.read_csv(f, delimiter="\t").dropna())
    else:
        df0 = pd.read_csv(f, delimiter="\t").dropna()
        df0["Elapsed time(s)"] += all_data[-1]["Elapsed time(s)"].iat[-1]
        all_data.append(df0)


df = pd.concat(all_data, ignore_index=True)

if not tqdm_disabled:
    print("Electrolyte Composition:")

    print(
        "Molarities (moles/L solution): {:.2f} M ZnCl~2~, {:.2f} M NH~4~Cl, {:.2f} M KI, {:.2f} M triethylene glycol, {:.2f} M H~2~O\n".format(
            molarity_ZnCl2, molarity_NH4Cl, molarity_KI, molarity_TriEG, molarity_H2O
        )
    )
    print(
        "Molalities (moles/kg solution): {:.2f} m ZnCl~2~, {:.2f} m NH~4~Cl, {:.2f} m KI, {:.2f} m triethylene glycol, {:.2f} m H~2~O\n".format(
            molality_ZnCl2, molality_NH4Cl, molality_KI, molality_TriEG, molality_H2O
        )
    )
    print("Density approx. {:.1f} g/mL\n".format(density))
    print(
        "Experiment length: {:.1f} hours".format(
            all_data[-1]["Elapsed time(s)"].iat[-1] / 3600.0
        )
    )


df["mean_current"] = df["Current(A)"].rolling(3).mean()
df["prev_current"] = df["mean_current"].shift(-1)
df["VChange"] = df["Potential(V)"].diff().abs()
df["is_change"] = (
    ((df["mean_current"] > 0) & (df["prev_current"] < 0))
    | ((df["mean_current"] < 0) & (df["prev_current"] > 0))
).astype(int)

idx_changes = list(df[df["is_change"] == 1].index)
idx_changes.append(len(df) - 1)

all_curves = []
idx_start = 0
for idx in tqdm(idx_changes, disable=tqdm_disabled):
    if len(df.iloc[idx_start:idx, :]) > 50:
        all_curves.append(df.iloc[idx_start:idx, :])
    idx_start = idx

results = []
n_curves = np.max([1, int(np.floor(len(all_curves) / 2))])

for CN in notebook.tnrange(n_curves, disable=tqdm_disabled):
    CURVE_N1 = CN * 2
    CURVE_N2 = CN * 2 + 1

    # Process charge data

    if sampling:
        N_TERM_POINTS = int(np.min([MIN_POINTS0, len(all_curves[CURVE_N1]) / 2.0]))
        MIN_POINTS = int(
            np.min([MIN_POINTS0, len(all_curves[CURVE_N1]) - N_TERM_POINTS * 2])
        )

        df0 = pd.concat(
            [
                all_curves[CURVE_N1].iloc[:N_TERM_POINTS],
                all_curves[CURVE_N1]
                .iloc[N_TERM_POINTS:-N_TERM_POINTS]
                .sample(n=MIN_POINTS),
                all_curves[CURVE_N1].iloc[-N_TERM_POINTS:],
            ]
        ).sort_values("Elapsed time(s)", ascending=True)
        df0 = df0[df0["VChange"] < DIFF_LIMIT]
    else:
        df0 = all_curves[CURVE_N1].copy()
    df0["mAh"] = np.abs(
        scipy.integrate.cumulative_trapezoid(
            df0["Current(A)"], df0["Elapsed time(s)"], initial=0
        )
        * 1000.0
        / 3600.0
    )
    total_energy0 = scipy.integrate.cumulative_trapezoid(
        df0["Current(A)"].abs() * df0["Potential(V)"],
        df0["Elapsed time(s)"],
        initial=0.0,
    )[-1]

    # Process discharge data
    if sampling:
        N_TERM_POINTS = int(np.min([MIN_POINTS0, len(all_curves[CURVE_N2]) / 2.0]))
        MIN_POINTS = int(
            np.min([MIN_POINTS0, len(all_curves[CURVE_N2]) - N_TERM_POINTS * 2])
        )
        df1 = pd.concat(
            [
                all_curves[CURVE_N2].iloc[:N_TERM_POINTS],
                all_curves[CURVE_N2]
                .iloc[N_TERM_POINTS:-N_TERM_POINTS]
                .sample(n=MIN_POINTS),
                all_curves[CURVE_N2].iloc[-N_TERM_POINTS:],
            ]
        ).sort_values("Elapsed time(s)", ascending=True)
        df1 = df1[df1["VChange"] < DIFF_LIMIT]
    else:
        df1 = all_curves[CURVE_N2].copy()

    df1["mAh"] = np.abs(
        scipy.integrate.cumulative_trapezoid(
            df1["Current(A)"], df1["Elapsed time(s)"], initial=0.0
        )
        * 1000.0
        / 3600.0
    )
    total_energy1 = scipy.integrate.cumulative_trapezoid(
        df1["Current(A)"].abs() * df1["Potential(V)"],
        df1["Elapsed time(s)"],
        initial=0.0,
    )[-1]

    CE = 100.0 * (df1["mAh"].iloc[-1] / df0["mAh"].iloc[-1])
    EE = 100.0 * (total_energy1 / total_energy0)
    VE = 100.0 * EE / CE
    results.append(
        {
            "Number": CN + 1,
            "CE": CE,
            "VE": VE,
            "EE": EE,
            "Charge_potential": df0["Potential(V)"].mean(),
            "Discharge_potential": df1["Potential(V)"].mean(),
            "Charge_stored": df1["mAh"].iloc[-1] / TOTAL_VOLUME,
            "Energy_density_discharge": total_energy1 / TOTAL_VOLUME / 3600.0 * 1000,
        }
    )

    # Save the modified DataFrames back to the all_curves list
    all_curves[CURVE_N1] = df0
    all_curves[CURVE_N2] = df1

results_df = pd.DataFrame(results)

if not tqdm_disabled:
    print(results_df)
    print("")
    print(results_df.mean())


# Color gradient for charge curves
charge_colors = [
    px.colors.sequential.Blues[int(i)]
    for i in np.linspace(3, len(px.colors.sequential.Blues) - 1, n_curves)
]
discharge_colors = [
    px.colors.sequential.Greys[int(i)]
    for i in np.linspace(3, len(px.colors.sequential.Greys) - 1, n_curves)
]


# Plot charge/discharge curves
fig1 = go.Figure()
for CN in range(n_curves):
    CURVE_N1 = CN * 2
    CURVE_N2 = CN * 2 + 1
    fig1.add_trace(
        go.Scatter(
            x=all_curves[CURVE_N1]["mAh"] / TOTAL_VOLUME,
            y=all_curves[CURVE_N1]["Potential(V)"],
            mode="lines",
            name=f"Charge {CN+1}",
            line=dict(color=charge_colors[CN], dash="solid"),
            showlegend=False,
        )
    )
    fig1.add_trace(
        go.Scatter(
            x=all_curves[CURVE_N2]["mAh"] / TOTAL_VOLUME,
            y=all_curves[CURVE_N2]["Potential(V)"],
            mode="lines",
            name=f"Discharge {CN+1}",
            line=dict(color=discharge_colors[CN], dash="solid"),
            showlegend=False,
        )
    )
fig1.update_layout(
    xaxis_title="Capacity (Ah/L)",
    yaxis_title="Potential (V)",
    legend=dict(orientation="h", yanchor="bottom", y=0.02, xanchor="right", x=0.99),
    hoverlabel=dict(
        bgcolor="white",
    ),
    xaxis=dict(range=[-1, 10]),
    yaxis=dict(range=[-.49, 1.8]),


)

fig1.add_trace(
    go.Scatter(
        x=[None],
        y=[None],
        mode="lines",
        line=dict(color=charge_colors[0], dash="solid"),
        name="Charge (cycle 1)",
    )
)
fig1.add_trace(
    go.Scatter(
        x=[None],
        y=[None],
        mode="lines",
        line=dict(color=charge_colors[-1], dash="solid"),
        name=f"Charge (cycle {n_curves})",
    )
)
fig1.add_trace(
    go.Scatter(
        x=[None],
        y=[None],
        mode="lines",
        line=dict(color=discharge_colors[0], dash="solid"),
        name="Discharge (cycle 1)",
    )
)
fig1.add_trace(
    go.Scatter(
        x=[None],
        y=[None],
        mode="lines",
        line=dict(color=discharge_colors[-1], dash="solid"),
        name=f"Discharge (cycle {n_curves})",
    )
)

fig1.show()
Figure 1: Charge/discharge curves
Code
# Plot efficiency
fig2 = px.scatter(
    results_df,
    x="Number",
    y=["VE", "CE", "EE"],
    labels={"value": "Efficiency (%)", "variable": "Metric"},
)
fig2.update_traces(mode="markers")


fig2.update_layout(
    yaxis=dict(range=[-10, 100]),
    legend=dict(
        orientation="v",
        yanchor="bottom",
        y=0.02,
        xanchor="right",
        x=0.99
    )
)


fig2.show()
Figure 2: Charge/discharge efficiencies
Code
fig5 = px.scatter(
    results_df,
    x="Number",
    y="Energy_density_discharge",
    labels={
        "Energy_density_discharge": "Energy Density on Discharge (Wh/L)",
        "Number": "Cycle Number",
    },
    range_y=[0,1.2*max(results_df["Energy_density_discharge"])]
)

max_val = results_df["Energy_density_discharge"].max()
mean_val = results_df["Energy_density_discharge"].mean()

fig5.add_hline(y=max_val, line_dash="dash", line_color="black", annotation_text="Max", annotation_position="top right",annotation_font_size = 10)
fig5.add_hline(y=mean_val, line_dash="dash", line_color="blue", annotation_text="Mean", annotation_position="top right",annotation_font_size = 10)
fig5.add_hline(y=0.8*max_val, line_dash="dash", line_color="red", annotation_text="80% Max", annotation_position="top right",annotation_font_size = 10)

fig5.show()
Figure 3: Discharge energy densities
Code
norm_charge = results_df["Charge_potential"] / results_df["Charge_potential"].iloc[0]
norm_discharge = results_df["Discharge_potential"] / results_df["Discharge_potential"].iloc[0]

fig6 = go.Figure()
fig6.add_trace(go.Scatter(
    x=results_df["Number"],
    y=norm_charge,
    mode="lines+markers",
    name="Charge Potential"
))
fig6.add_trace(go.Scatter(
    x=results_df["Number"],
    y=norm_discharge,
    mode="lines+markers",
    name="Discharge Potential"
))
fig6.update_layout(
    xaxis_title="Cycle Number",
    yaxis_title="Normalized Potential",
    legend=dict(
        orientation="v",
        yanchor="top",
        y=0.95,
        xanchor="left",
        x=0.05
    )
)

fig6.show()
Figure 4: Average charge and discharge potentials normalized to first cycle
Code
table_df = (
    results_df.describe().loc[["mean", "std"]]
    .round(decimals=1)
    .drop(columns=["Number", "Charge_potential", "Discharge_potential"])
    .rename(
        columns={
            "CE": "Coulombic Efficiency (%)",
            "EE": "Energy Efficiency (%)",
            "VE": "Voltaic Efficiency (%)",
            "Charge_stored": "Discharge Capacity (Ah/L)",
            "Energy_density_discharge": "Energy Density (Wh/L)",
        }
    )
)

# Bar chart of efficiencies with error bars
eff_cols = ["Coulombic Efficiency (%)", "Voltaic Efficiency (%)", "Energy Efficiency (%)"]
eff_labels = ["Coulombic", "Voltaic", "Energy"]

means = table_df.loc["mean", eff_cols].values
stds = table_df.loc["std", eff_cols].values
Code
fig6 = go.Figure()
fig6.add_trace(go.Bar(
    x=eff_labels,
    y=means,
    error_y=dict(type="data", array=stds, visible=True),
    name="Efficiency",
    marker_color=["#1f77b4", "#ff7f0e", "#2ca02c"]
))
fig6.update_layout(
    yaxis_title="Efficiency (%)",
    yaxis=dict(range=[0, 100])
)
fig6.show()
Figure 5: Mean efficiency values with standard deviation
Code
cap_cols = ["Discharge Capacity (Ah/L)"]
cap_labels = ["Discharge Capacity"]

cap_means = table_df.loc["mean", cap_cols].values
cap_stds = table_df.loc["std", cap_cols].values

ed_cols = ["Energy Density (Wh/L)"]
ed_labels = ["Energy Density"]

ed_means = table_df.loc["mean", ed_cols].values
ed_stds = table_df.loc["std", ed_cols].values

fig_combined = make_subplots(rows=1, cols=2)

fig_combined.add_trace(
    go.Bar(
        x=cap_labels,
        y=cap_means,
        error_y=dict(type="data", array=cap_stds, visible=True),
        name="Capacity",
        marker_color="#1f77b4"
    ),
    row=1, col=1
)

fig_combined.add_trace(
    go.Bar(
        x=ed_labels,
        y=ed_means,
        error_y=dict(type="data", array=ed_stds, visible=True),
        name="Energy Density",
        marker_color="#2ca02c"
    ),
    row=1, col=2
)
top = max(max(cap_means + cap_stds), max(ed_means + ed_stds))*1.1
fig_combined.update_layout(
    yaxis=dict(title="Discharge Capacity (Ah/L)"),
    yaxis2=dict(title="Energy Density (Wh/L)", anchor="x2", overlaying="y", side="left"),
    yaxis_range=[0, top],
    yaxis2_range=[0, top],
    showlegend=False
)
fig_combined.show()
Figure 6: Mean discharge capacity and energy density values with standard deviation

Citation

BibTeX citation:
@online{smith2026,
  author = {Smith, Kirk Pollard},
  title = {Lab {Notebook} {Entry} \#15},
  date = {2026-04-18},
  url = {https://dualpower.supply/posts/lab-notebook-15/},
  langid = {en}
}
For attribution, please cite this work as:
K.P. Smith, Lab Notebook Entry #15, (2026). https://dualpower.supply/posts/lab-notebook-15/.