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**SERIES AND PARALLEL CONNECTIONS OF RESISTORS**

A conducting material (e.g., a wire) of a particular resistance meant for use in a circuit is called a resistor. A resistor is sometimes simply referred to as a resistance. It is represented by the symbol . Two or more resistors can be connected in series, in parallel or in a manner that is a combination of these two.

**Series Connection of Resistors**

Two or more resistors are said to be connected in series if the current flowing through one also flows through the rest.

The total potential difference across the combination of resistors connected in series is equal to the sum of the potential differences across the individual resistors.

V = V_{1 }+ V_{2 }+ V_{3}

**Equivalent resistance in series connection**

Figure (a) shows three resistors of resistances R_{1}, R_{2} and R_{3} connected in series. The cell connected across the combination maintains a potential difference V across the combination. The current through the cell is i. The same current i flows through each resistor.

Let us replace the combination of resistors by a single resistor R_{eq} such that the current does not change, i.e., it remains i. This resistance is called the **equivalent resistance** of the combination, and its value is given by Ohm's law as R_{eq} = V / i

Thus V = i R_{eq. }

The potential differences V_{1} , V_{2} and V_{3} across the resistors R_{1} , R_{2} and R_{3} respectively are given by

Ohm's law as : V_{1} = iR_{1} , V_{2 }= iR_{2} , V_{3} = iR_{3}

Since the resistors are in series, V = V_{1} + V_{2} + V_{3}

Substituting the values of the potential differences in the above equation,

iR_{eq} = iR_{1} + iR_{2} + iR_{3}

or iR_{eq} = i(R_{1} +R_{2} +R_{3})

or R_{eq} = R_{1} + R_{2} + R_{3}

Similarly, for n resistors connected in series,**Equivalent resistance of resistors in series : R _{eq} = R_{1} + R_{2} + R_{3 }+ .... R_{n}**

**Parallel Connection of Resistors**

The total current flowing into the combination is equal to the sum of the currents passing through the individual resistors.**i = i _{1} + i_{2} + i_{3}**

If resistors are connected in such a way that the same potential difference gets applied to each of them, they are said to be connected in parallel.

**Equivalent resistance in parallel connection**

Figure (a) shows three resistors of resistances R_{1},_{ } R_{2} and R_{3} connected in parallel across the points A and B. The cell connected across these two points maintains a potential difference V across each resistor. The current through the cell is i. It gets divided at A into three parts i_{1}, i_{2} and i_{3}, which flow through R_{1}, R_{2} and R_{3} respectively.

Let us replace the combination of resistors by an equivalent resistor R_{eq} such that the current i in the circuit does not change (Fig). The equivalent resistance is given by Ohm's law as R_{eq} = V/i.

Thus,

The currents i_{1} , i_{2} and i_{3} through the resistors R_{1}, R_{2} and R_{3} respectively are given by Ohm's law as

Since the resistors are in parallel,

i = i_{1} + i_{2} + i_{3}

Substituting the values of the currents in the above equation,

Similarly, if there are n resistors connected in parallel, their equivalent resistance R_{eq} is given by

**Equivalent Resistance of resistors in parallel:**

For two resistances R_{1} and R_{2} connected in parallel,

The equivalent resistance in a parallel connection is less than each of the resistances.

When a resistance is joined parallel to a comparatively smaller resistance, the equivalent resistance is very close to the value of the smaller resistance.

**Note: **If a resistor connected in series with others is removed or fails, the current through each resistor becomes zero. On the other hand, if a resistor connected in parallel with others fails or is removed, the current continues to flow through the other resistors.

**Distribution of Current in Two Resistors in Parallel**

Consider the circuit in fig. The resistors R_{1} and R_{2} are connected in parallel. The current *i* gets distributed in the two resistors.

i = i_{1} + i_{2} .....(i)

Applying Ohm's law to the resistor R_{1 }

V_{A} - V_{B} =R_{1}i_{1}Â· .....(ii)

And applying Ohm's law to the resistor R_{2}

V_{A} - V_{B} = R_{2}i_{2} .... (iii)

From (ii) and (iii), R_{1}i_{1} = R_{2}i_{2} or

Substituting for i_{2} in (i), we have

or

Similarly,

Thus,

The current through each branch in a parallel combination of resistors is inversely proportional to its resistance.

**Devices in Series and Parallel**

You must have seen tiny bulbs strung together for decorating buildings during festivals like Diwali, and occasions like marriages, etc. These bulbs are connected in series, and the mains voltage is applied to the combination. The potential difference (V) of the mains gets divided across the bulbs (V = V_{1} + V_{2} + V_{3} + ... ). So, a small potential difference exists across each bulb, close to that required to make the bulb work. However, the same current flows through all the bulbs. So, if one bulb goes bad, the current through it stops, and this stops the current through the rest of the bulbs as well. To make the chain of lights work, we have to find and replace the defective bulb. This problem does not occur with the lights in our house. That is because **in houses, lights, fans, etc., are connected in parallel**. In parallel connection, the same mains voltage gets applied to each device, but the current through each is different. If one of them goes bad, the current in the other branches of the parallel connection does not stop. Another advantage of parallel connection is that, unlike series connection, each device can draw a different current, as per its requirement.

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