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    • https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electricity_and_Magnetism_(Tatum)/04%3A_Batteries_Resistors_and_Ohm's_Law/4.05%3A_Conductors_in_Parallel
      \(\text{FIGURE IV.3}\) \[G=G_1+G_2+G_3.\label{4.5.1}\] That is to say \[\frac{1}{R} = \frac{1}{R_1}+\frac{1}{R_2}+\frac{1}{R_3}.\label{4.5.2}\] The potential difference is the same across each. The cu...\(\text{FIGURE IV.3}\) \[G=G_1+G_2+G_3.\label{4.5.1}\] That is to say \[\frac{1}{R} = \frac{1}{R_1}+\frac{1}{R_2}+\frac{1}{R_3}.\label{4.5.2}\] The potential difference is the same across each. The current is greatest through the largest conductance – i.e. through the smallest resistance.

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