Given,
κ = 1.237 × 10−2 S m−1, c = 0.001 M
Then, κ = 1.237 × 10−4 S cm−1, c1⁄2 = 0.0316 M1/2
\(\begin{array}{l}\Lambda_m =\frac{k}{c}\end{array} \)
\(\begin{array}{l}=\frac{1.237 \times 10^{ -4 } S\;cm^{-1} }{0.001 \; mol\; \; L^{ -1 }}\times \frac{1000\;cm^{-1}}{L}\end{array} \)
= 123.7 S cm2 mol−1
Given,
κ = 11.85 × 10−2 S m−1, c = 0.010M
Then, κ = 11.85 × 10−4 S cm−1, c1⁄2 = 0.1 M1/2
\(\begin{array}{l}\Lambda_m =\frac{k}{c}\end{array} \)
\(\begin{array}{l}=\frac{11.85 \times 10^{ -4 } S\;cm^{-1} }{0.010 \; mol\; \; L^{ -1 }}\times \frac{1000\;cm^{-1}}{L}\end{array} \)
= 118.5 S cm2 mol−1
Given,
κ = 23.15 × 10−2 S m−1, c = 0.020 M
Then, κ = 23.15 × 10−4 S cm−1, c1/2 = 0.1414 M1/2
\(\begin{array}{l}\Lambda_m =\frac{k}{c}\end{array} \)
\(\begin{array}{l}=\frac{23.15 \times 10^{ -4 } S\;cm^{-1} }{0.020 \; mol\; \; L^{ -1 }}\times \frac{1000\;cm^{-1}}{L}\end{array} \)
= 115.8 S cm2 mol−1
Given,
κ = 55.53 × 10−2 S m−1, c = 0.050 M
Then, κ = 55.53 × 10−4 S cm−1, c1/2 = 0.2236 M1/2
\(\begin{array}{l}\Lambda_m =\frac{k}{c}\end{array} \)
\(\begin{array}{l}=\frac{106.74 \times 10^{ -4 } S\;cm^{-1} }{0.050 \; mol\; \; L^{ -1 }}\times \frac{1000\;cm^{-1}}{L}\end{array} \)
= 111.1 1 S cm2 mol−1
Given,
κ = 106.74 × 10−2 S m−1, c = 0.100 M
Then, κ = 106.74 × 10−4 S cm−1, c1/2 = 0.3162 M1/2
\(\begin{array}{l}\Lambda_m =\frac{k}{c}\end{array} \)
\(\begin{array}{l}=\frac{106.74 \times 10^{ -4 } S\;cm^{-1} }{0.100 \; mol\; \; L^{ -1 }}\times \frac{1000\;cm^{-1}}{L}\end{array} \)
= 106.74 S cm2 mol−1
Now, we have the following data:

Since the line interrupts
\(\begin{array}{l}\Lambda_m\end{array} \)
2−1\(\begin{array}{l}\Lambda^0_m\end{array} \)
2−1