what is parrellel and series arrangement of electric particle
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Circuits consisting of just one battery and one load resistance are very simple to analyze, but they are not often found in practical applications. Usually, we find circuits where more than two components are connected together.
There are two basic ways in which to connect more than two circuit components: series and parallel. First, an example of a series circuit:
In the Attachment
Here, we have three resistors (labeled R1, R2, and R3), connected in a long chain from one terminal of the battery to the other. (It should be noted that the subscript labeling—those little numbers to the lower-right of the letter “R”—are unrelated to the resistor values in ohms. They serve only to identify one resistor from another.) The defining characteristic of a series circuit is that there is only one path for electrons to flow. In this circuit the electrons flow in a counter-clockwise direction, from point 4 to point 3 to point 2 to point 1 and back around to 4.
Now, let’s look at the other type of circuit, a parallel configuration:
In the Attachment
Again, we have three resistors, but this time they form more than one continuous path for electrons to flow. There’s one path from 8 to 7 to 2 to 1 and back to 8 again. There’s another from 8 to 7 to 6 to 3 to 2 to 1 and back to 8 again. And then there’s a third path from 8 to 7 to 6 to 5 to 4 to 3 to 2 to 1 and back to 8 again. Each individual path (through R1, R2, and R3) is called a branch.
The defining characteristic of a parallel circuit is that all components are connected between the same set of electrically common points. Looking at the schematic diagram, we see that points 1, 2, 3, and 4 are all electrically common. So are points 8, 7, 6, and 5. Note that all resistors as well as the battery are connected between these two sets of points.
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Here is your answer
Circuits consisting of just one battery and one load resistance are very simple to analyze, but they are not often found in practical applications. Usually, we find circuits where more than two components are connected together.
There are two basic ways in which to connect more than two circuit components: series and parallel. First, an example of a series circuit:
In the Attachment
Here, we have three resistors (labeled R1, R2, and R3), connected in a long chain from one terminal of the battery to the other. (It should be noted that the subscript labeling—those little numbers to the lower-right of the letter “R”—are unrelated to the resistor values in ohms. They serve only to identify one resistor from another.) The defining characteristic of a series circuit is that there is only one path for electrons to flow. In this circuit the electrons flow in a counter-clockwise direction, from point 4 to point 3 to point 2 to point 1 and back around to 4.
Now, let’s look at the other type of circuit, a parallel configuration:
In the Attachment
Again, we have three resistors, but this time they form more than one continuous path for electrons to flow. There’s one path from 8 to 7 to 2 to 1 and back to 8 again. There’s another from 8 to 7 to 6 to 3 to 2 to 1 and back to 8 again. And then there’s a third path from 8 to 7 to 6 to 5 to 4 to 3 to 2 to 1 and back to 8 again. Each individual path (through R1, R2, and R3) is called a branch.
The defining characteristic of a parallel circuit is that all components are connected between the same set of electrically common points. Looking at the schematic diagram, we see that points 1, 2, 3, and 4 are all electrically common. So are points 8, 7, 6, and 5. Note that all resistors as well as the battery are connected between these two sets of points.
Hoping it helps
Thanks......
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=> parallel :- Resistance is decreased. ,Same potential difference flows through all parts or through each resistor in a circuit , Current across each resistor is different ,Total current across circuit is equal to the sum of reciprocal of individual resistor.
formula :- 1/R(p) = 1/R1 + 1/R2+ 1/R3 + ...
Total resistance in parallel is always smaller than the value of each individual resistor.
=> series :- Resistance is increased ,Same current flows through all parts or through each resistor in a circuit ,Potential difference across each resistor is different , Total potential difference across the circuit is equal to sum of all potential differences across each resistor.
formula :- R(s) = R1 + R2 + R3 + ...
total resistance in series is always greater than the value of each individual resistor.
formula :- 1/R(p) = 1/R1 + 1/R2+ 1/R3 + ...
Total resistance in parallel is always smaller than the value of each individual resistor.
=> series :- Resistance is increased ,Same current flows through all parts or through each resistor in a circuit ,Potential difference across each resistor is different , Total potential difference across the circuit is equal to sum of all potential differences across each resistor.
formula :- R(s) = R1 + R2 + R3 + ...
total resistance in series is always greater than the value of each individual resistor.
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