write property of parallels of parallel resistor and series resistor ?
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Resistors in Series and in Parallel
Resistors are probably the most commonly occurring components in electronic circuits. Practical circuits often contain very complicated combinations of resistors. It is, therefore, useful to have a set of rules for finding the equivalent resistance of some general arrangement of resistors. It turns out that we can always find the equivalent resistance by repeated application of two simple rules. These rules relate to resistors connected in series and in parallel.
Figure 18: Two resistors connected in series.
Consider two resistors connected in series, as shown in Fig. 18. It is clear that the same current  flows through both resistors. For, if this were not the case, charge would build up in one or other of the resistors, which would not correspond to a steady-state situation (thus violating the fundamental assumption of this section). Suppose that the potential drop from point  to point  is . This drop is the sum of the potential drops  and  across the two resistors  and , respectively. Thus,
(135)
According to Ohm's law, the equivalent resistance  between  and  is the ratio of the potential drop  across these points and the current  which flows between them. Thus,
(136)
giving
(137)
Here, we have made use of the fact that the current  is common to all three resistors. Hence, the rule is
The equivalent resistance of two resistors connected in series is the sum of the individual resistances.
For  resistors connected in series, Eq. (137) generalizes to .
Figure 19: Two resistors connected in parallel.
Consider two resistors connected in parallel, as shown in Fig. 19. It is clear, from the figure, that the potential drop across the two resistors is the same. In general, however, the currents  and which flow through resistors  and , respectively, are different. According to Ohm's law, the equivalent resistance between  and  is the ratio of the potential drop  across these points and the current  which flows between them. This current must equal the sum of the currents  and  flowing through the two resistors, otherwise charge would build up at one or both of the junctions in the circuit. Thus,
(138)
It follows that
(139)
giving
(140)
Here, we have made use of the fact that the potential drop  is common to all three resistors. Clearly, the rule is
The reciprocal of the equivalent resistance of two resistances connected in parallel is the sum of the reciprocals of the individual resistances.
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Resistors are probably the most commonly occurring components in electronic circuits. Practical circuits often contain very complicated combinations of resistors. It is, therefore, useful to have a set of rules for finding the equivalent resistance of some general arrangement of resistors. It turns out that we can always find the equivalent resistance by repeated application of two simple rules. These rules relate to resistors connected in series and in parallel.
Figure 18: Two resistors connected in series.
Consider two resistors connected in series, as shown in Fig. 18. It is clear that the same current  flows through both resistors. For, if this were not the case, charge would build up in one or other of the resistors, which would not correspond to a steady-state situation (thus violating the fundamental assumption of this section). Suppose that the potential drop from point  to point  is . This drop is the sum of the potential drops  and  across the two resistors  and , respectively. Thus,
(135)
According to Ohm's law, the equivalent resistance  between  and  is the ratio of the potential drop  across these points and the current  which flows between them. Thus,
(136)
giving
(137)
Here, we have made use of the fact that the current  is common to all three resistors. Hence, the rule is
The equivalent resistance of two resistors connected in series is the sum of the individual resistances.
For  resistors connected in series, Eq. (137) generalizes to .
Figure 19: Two resistors connected in parallel.
Consider two resistors connected in parallel, as shown in Fig. 19. It is clear, from the figure, that the potential drop across the two resistors is the same. In general, however, the currents  and which flow through resistors  and , respectively, are different. According to Ohm's law, the equivalent resistance between  and  is the ratio of the potential drop  across these points and the current  which flows between them. This current must equal the sum of the currents  and  flowing through the two resistors, otherwise charge would build up at one or both of the junctions in the circuit. Thus,
(138)
It follows that
(139)
giving
(140)
Here, we have made use of the fact that the potential drop  is common to all three resistors. Clearly, the rule is
The reciprocal of the equivalent resistance of two resistances connected in parallel is the sum of the reciprocals of the individual resistances.
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Please mark me brainlist
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