Layer (i)

Bottom (b)

~mean (m)

Top (t)

Height ( $r/R_{\odot }$ )

1.16

1.19

1.23

HomgR [Volume]

$4l_b\pi l_b^2$

$4\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_m-r_b\right]\right)}^3$

$4\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_t-r_b\right]\right)}^3$

HomgR [Section]

$\pi l_b^2$

$\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_m-r_b\right]\right)}^2$

$\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_t-r_b\right]\right)}^2$

HomgR e-number/cm³

$N_{b}4l_b\pi l_b^2$

$N_{m}4\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_m-r_b\right]\right)}^3$

$N_{t}4\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_t-r_b\right]\right)}^3$

HomgR number moles

$\frac{N_{b}4l_b\pi l_b^2}{6.022\times {10}^{23}}$

$\frac{N_{m}4\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_m-r_b\right]\right)}^3}{6.022\times {10}^{23}}$

$\frac{N_{t}4\pi {\left(l_b+\text{<menclose notation="updiagonalstrike"> c </menclose>}\left[r_t-r_b\right]\right)}^3}{6.022\times {10}^{23}}$

$\ln \left(\frac{N_i/r_i^2}{N_b/r_b^2}\right)RT$

_

−3.377 × 10⁶

−6.093 × 10⁶

$W_g\left(r-r_b\right)\left[\text{J}\right]$

_

−4.040 × 10⁵

−8.092 × 10⁵

$W_M\left(r-r_b\right)\left[\text{J}\right]$

(Equation (21))

_

−2.973 × 10⁶

−5.284 × 10⁶