A dissipated power, $P$, in a resistor can be described by $P=R \cdot I^2$, where $R$ is the resistance, in ohms, and $I$ is the current, measured in amps, passing through the resistor. Let a fuzzy set R be defined on the universe $x_1=\{10,20,30,40,50\}$ ohms and a fuzzy set $I$ be defined on the universe $x_2=\{0,1,2,3\} \mathrm{amps}$. We wish to map elements of these fuzzy sets to the dissipated power universe, y , under the relation $P=R \cdot I^2$. We have a medium resistance given by
$$
\underset{R}{R}=\left\{\frac{0.3}{10}+\frac{0.9}{20}+\frac{1}{30}+\frac{0.8}{40}+\frac{0.4}{50}\right\}=\text { "medium resistance" }
$$
and a low current given by
$$
\mathrm{I}=\left\{\frac{0.5}{0}+\frac{1}{1}+\frac{0.4}{2}+\frac{0.1}{3}\right\}=\text { "low current" }
$$
Using the discretized form of the extension principle, determine the membership values for $P$.