For the series combination of three resistors establish the relation: |
\[\mathbf{R = }{{\mathbf{R}}_{\mathbf{1}}}\mathbf{+ }{{\mathbf{R}}_{\mathbf{2}}}\mathbf{+ }{{\mathbf{R}}_{\mathbf{3}}}\] |
where the symbols have their usual meanings. |
Calculate the equivalent resistance of the combination of three resistors of \[\mathbf{6}\,\mathbf{\Omega ,}\,\mathbf{9}\,\mathbf{\Omega }\] and \[\mathbf{18}\,\mathbf{\Omega }\] joined in parallel. |
Answer:
Same current (I) flows through different resistances, when these are joined in series, as shown in the figure. Let R be the combined resistance, then \[V=IR\] Also, \[{{V}_{1}}=I{{R}_{1}},\text{ }{{V}_{2}}=I{{R}_{2}},{{V}_{3}}=I{{R}_{3}}\] \[\because \] \[V={{V}_{1}}+{{V}_{2}}+{{V}_{3}}\] \[\therefore \] \[IR=I{{R}_{1}}+I{{R}_{2}}+I{{R}_{3}}\] \[\Rightarrow \] \[IR=I({{R}_{1}}+{{R}_{2}}+{{R}_{3}})\] \[R={{R}_{1}}+{{R}_{2}}+{{R}_{3}}\] Now, \[{{R}_{1}}=6\,\Omega ,\text{ }{{R}_{2}}=\,9\,\Omega ,\text{ }{{R}_{3}}=18\,\Omega \] In parallel combination, \[\frac{1}{R}=\frac{1}{{{R}_{1}}}+\frac{1}{{{R}_{2}}}+\frac{1}{{{R}_{3}}}\] \[\Rightarrow \] \[\frac{1}{R}=\frac{1}{6}+\frac{1}{9}+\frac{1}{18}=\frac{3+2+1}{18}\] \[=\frac{6}{18}=\frac{1}{3}\] \[\Rightarrow \] \[\frac{1}{R}=\frac{1}{3}\] \[\Rightarrow \] \[R=3\,\Omega \]
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