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Question: Three resistances, \( 1\Omega ,2\Omega ,3\Omega \) are connected in Series. What is the total resist...

Three resistances, 1Ω,2Ω,3Ω1\Omega ,2\Omega ,3\Omega are connected in Series. What is the total resistance of the combination?
If the combination is connected to a 12V12{V} battery of negligible internal resistance, obtain the potential drop across each resistor.

Explanation

Solution

The effective resistance of n Resistors of Resistances R1,R2,R3Rn{R_1},{R_2},{R_3} \cdot \cdot \cdot {R_n}is Reff=R1+R2+R3++Rn{R_{eff}} = {R_1} + {R_2} + {R_3} + \cdot \cdot \cdot + {R_n} . Also, when the current in a circuit is the same, the Resistances and Voltage across them follow a direct proportion.

Complete step-by-step answer:
We know that when three resistors- R1{R_1} , R2{R_2} , R3{R_3} are connected in series, their effective resistance is given by : Reff=R1+R2+R3{R_{eff}} = {R_1} + {R_2} + {R_3}
Here, Since the resistances - R1=1Ω{R_1} = 1\Omega , R2=2Ω{R_2} = 2\Omega and R3=3Ω{R_3} = 3\Omega Reff=1Ω+2Ω+3Ω=6Ω{R_{eff}} = 1\Omega + 2\Omega + 3\Omega = 6\Omega .

Now let's consider this combination of resistors being connected in series with a cell of 12V12V emf.

Since the cell is assumed to have zero internal resistance, the ends of the combination are directly connected to 12V12V emf and hence, the potential difference across the combination is 12V12V .
Let us now find the current passing through this circuit. Since the effective resistance of the combination is 6Ω6\Omega , The current in the circuit can be found using ohm's law as: I=VRI = \dfrac{V}{R} Substituting values of VV and RR gives us : I=126=2AI = \dfrac{{12}}{6} = 2A
This 2A2A current is flowing through all three resistors since they are connected parallel.
Now, we are to find the potential drop across each resistor. So let the potential drop across resistors R1{R_1} , R2{R_2} , R3{R_3} be V1{V_1} , V2{V_2} , V3{V_3} respectively. Now ohm's Law tells us that the voltages V1{V_1} , V2{V_2} and V3{V_3} are related to the current II flowing through them and their resistances as-

V=I×RV = I \times R So V1=I×R1=2×1=2V{V_1} = I \times {R_1} = 2 \times 1 = 2V V2=I×R2=2×2=4V{V_2} = I \times {R_2} = 2 \times 2 = 4V V3=I×R3=2×3=6V{V_3} = I \times {R_3} = 2 \times 3 = 6V So the potential difference across R1{R_1} is 2V2V , R2{R_2} is 4V4V , R3{R_3} is 6V6V .

Additional Information:
we see that summing the voltage across all resistors - 2V+4V+6V2V + 4V + 6V , we get the emf of the cell. This is true for all closed loops in a Resistive circuit and called Kirchoff's voltage rule. Also, we can see that since the current is the same in a series circuit, Ohm's law simplifies to VRV \propto R . So the total voltage 12V12V gets divided among the resistors in the direct ratio of their Resistance.

Note: For competitive examinations, calculations have to be simplified and hence, we can use the Direct proportionality between VV and RR to find the Voltages.
Since V1:V2:V3::1:2:3{V_1}:{V_2}:{V_3}::1:2:3
V1=11+2+3Vtot{V_1} = \dfrac{1}{{1 + 2 + 3}}{V_{tot}}
V1=1612V=2V{V_1} = \dfrac{1}{6}12V = 2V
Similarly,
V2=2612V=4V{V_2} = \dfrac{2}{6}12V = 4V
V3=3612V=6V{V_3} = \dfrac{3}{6}12V = 6V