Step 1: Write the BET equation in linear form.
The BET adsorption isotherm, in the linear form used for this plot, is
\[
\frac{z}{(1-z)V} = \frac{1}{V_mC} + \frac{C-1}{V_mC}\,z
\]
So intercept \(= \dfrac{1}{V_mC}\) and slope \(=\dfrac{C-1}{V_mC}\), where \(V_m\) is the monolayer volume of gas (per gram of adsorbent here, since the sample is 1.0 g) and \(C\) is the BET constant.
Step 2: Add slope and intercept to eliminate \(C\).
\[
\mathrm{slope}+\mathrm{intercept} = \frac{C-1}{V_mC}+\frac{1}{V_mC} = \frac{C}{V_mC} = \frac{1}{V_m}
\]
\[
V_m = \frac{1}{\mathrm{slope}+\mathrm{intercept}} = \frac{1}{(6\times10^{-4})+(4\times10^{-6})} = \frac{1}{6.04\times10^{-4}}
\]
\[
V_m = 1655.63\ \mathrm{mm^3}
\]
This is the monolayer volume of \(\mathrm{N_2}\) gas (at the measurement conditions) adsorbed on the 1.0 g sample.
Step 3: Convert \(V_m\) into the number of molecules in the monolayer.
Given: 1 mm\(^3\) of \(\mathrm{N_2}\) gas corresponds to \(2.7\times10^{16}\) molecules.
\[
N = V_m \times 2.7\times10^{16} = 1655.63 \times 2.7\times10^{16} = 4.4702\times10^{19}\ \mathrm{molecules}
\]
Step 4: Convert molecule count to surface area.
Each \(\mathrm{N_2}\) molecule covers \(0.16\ \mathrm{nm^2} = 0.16\times10^{-18}\ \mathrm{m^2}\).
\[
A = N \times 0.16\times10^{-18}\ \mathrm{m^2} = (4.4702\times10^{19})(1.6\times10^{-19}) = 7.1523\ \mathrm{m^2}
\]
Step 5: State per-gram surface area.
Since this area belongs to the 1.0 g adsorbent sample used in the measurement, the specific surface area is directly \(7.1523\ \mathrm{m^2\,g^{-1}}\).
Final Answer:
Rounded to one decimal place, the BET surface area is
\[ \boxed{7.2\ \mathrm{m^2\,g^{-1}}} \]