Introduction to Series-Parallel Circuit Analysis
Understanding series-parallel resistor circuits is key for solving complex electrical networks. This guide details methods to find equivalent resistance, currents, node potentials, and power distribution in circuits with multiple resistors and a single battery. For foundational concepts, refer to Understanding Circuits: Key Concepts and Theories.
Step 1: Calculate Equivalent Resistance
- Identify series and parallel groups:
- Resistors in series are added directly (R_eq = R1 + R2 + ...).
- Resistors in parallel use the formula 1/R_eq = 1/R1 + 1/R2 + ...
- Simplify gradually:
- Combine series resistors first.
- Replace equal-value parallel resistors with half the resistance.
- Use the parallel resistance formula for different values. For a comprehensive explanation of resistors and related components, see Understanding Conductors and Capacitors in Electric Circuits.
Step 2: Determine Total Circuit Current
- Use Ohm's Law: I_total = V_battery / R_eq.
- This current flows through series branches uniformly. For a deeper grasp of current and potential difference, check Understanding Electricity: The Basics of Current, Potential Difference, and Resistance.
Step 3: Assign Node Potentials
- Set a reference point (e.g., point A) at 0 V.
- Moving through the battery from negative to positive terminal increases potential by battery voltage.
- Voltage drops occur across resistors following the direction of current.
- Calculate potential at each node using V_node = V_previous - (I × R) or V_previous + (I × R) when moving opposite current flow.
Step 4: Calculate Currents Through Branches
- Apply Kirchhoff's Current Law at junctions: total current entering equals total current leaving.
- For parallel branches, calculate individual currents using:
- Current division rule: I_branch = I_total × (R_other / (R_branch + R_other))
- Use voltage differences and Ohm’s Law (I = V / R) where potentials differ. These principles are further detailed in Understanding LCR Circuits: A Guide to AC Circuit Theory, which, although oriented towards AC, provides useful insights on current division and node analysis.
Step 5: Verify with Power Calculations
- Power absorbed by each resistor: P = I^2 × R.
- Power delivered by battery: P = V × I_total.
- Sum of resistor power absorptions should equal power delivered by battery, confirming solution accuracy.
Example Problem Highlights
- Combining three series resistors (5 Ω, 3 Ω, 2 Ω) into one 10 Ω resistor.
- Simplifying parallel resistors of equal value by halving resistance.
- Calculating potentials at nodes A through F step-by-step.
- Using currents and potentials to find branch currents in a more complex circuit with an added resistor.
- Applying formulas for current division when parallel resistor values differ.
Tips for Effective Circuit Analysis
- Label all nodes and assign reference potentials early.
- Break down complex circuits into simpler series and parallel parts.
- Carefully track voltage rises and drops following current flow direction.
- Use Kirchhoff’s laws to handle branching points.
- Double-check answers with power balance as a verification step.
By mastering these steps and principles, you can confidently solve any series-parallel resistor circuit for equivalent resistance, currents, voltages, and power distributions.
in this video we're going to talk about how to solve any type of series parallel combination circuit like this one
now the first thing you want to do is you want to calculate the equivalent resistance
so notice that these three resistors are in series with each other and so the equivalent resistance of
those three is going to be five plus three plus two which is ten so we can replace those three resistors
with a single 10 ohm resistor now every other part of the circuit is
going to remain the same initially so this is 10 ohms and this is still 10 this is still 5
and that's still 10. now notice that we have two resistors in parallel
they're directly across from each other and they have the same resistance whenever you have two parallel resistors
with the same value the equivalent resistance is simply half of that value
so individually they're both 10 so the equivalent resistance is going to be 5. so we can get rid of this
and replace it with a 5 ohm resistor so now these three are
in series with each other so then we could just add them 10 plus 5 plus 5 is 20.
so the equivalent resistance in the circuit is 20 ohms
once you have the equivalent resistance you could find the current that
is delivered from the battery and you could use v equals ir
so if you rearrange this equation to solve for i the current is going to be the voltage
of the battery divided by the total resistance or the equivalent resistance so the voltage of the battery is 60
volts in this example and the equivalent resistance is 20 ohms so 60 divided by 20 is 3 amps so that's
the current that leaves the battery now let's call this position a
let's say this is b c d
e and f now in order to calculate the current
that's flowing through each resistor it's helpful to know the potential at each of these points
and we're going to say at point a the potential is zero volts so now if we travel in this direction
from a to b we're going towards the positive terminal of the battery
and the battery increases the energy of the circuit because it delivers power to the circuit so as you go from a to b
it's going to be a voltage lift of 60 volts so the potential at b
is 60 volts now something else they need to know is that whenever or current
flows through a resistor the current flows from a high potential to a low potential
so we have the current of 3 amps it's flowing through the 10 ohm resistor
so let's call that just 3 amps so that means this is positive
and this is negative so c is at a lower potential than b so to calculate the potential at c
it's going to be the potential at b minus i r
because c is lower than b so the potential at b is 60 volts the current flowing through the 10 ohm
resistor is 3 amps multiplied by 10 so 3 times 10 is the voltage drop of 30 and then 60 minus 30
tells us that the potential at c is 30 volts now let's go from a to f
now this 3 amp current which flows through the battery also flows through the 5 ohm resistor
because this path here they're all in series whenever there's only a single path for the current to
flow you have a series path and the current flowing through that path is the same everywhere along that path
so what this tells us is that 3 amps of current flows through the 5 ohm resistor
and current always flows from a high potential to a low potential
so as we travel from a to f that's going to be a voltage lift because we're going from the negative
side to the positive side so anytime you go against the current the electric potential is increasing
if you're following the current like we did over here the potential decreased so to calculate the potential at f is
going to be the potential at a plus i r because we're going towards a higher
potential so this is going to be plus instead of minus
so the potential at a is zero the current flowing through the 5 ohm resistor is 3 amps times 5
so the potential at f is going to be 15 volts now let's get rid of this
and let's focus on the 10 ohm resistor because we now have the potential across c and
across f so we can calculate the current flowing through that resistor
now voltage is equal to current times resistance based on ohm's law
and voltage is also known as the potential difference between two points so we know that the current is flowing
in this direction and also current flows from a high potential to a low potential
so the potential at c is higher than the potential at a so the voltage across that resistor is
going to be the potential at c minus the potential at f
and that's equal to the current times the resistance so the potential at c is 30 the
potential at f is 15 and we don't know the current yet but the resistance is 10. so 30 minus 15
will give us a voltage of 15 volts across that resistor and so 15 divided by 10
is 1.5 so that's the current that flows through the 5 ohm resistor
so now we could calculate the current that flows through the other branch so let's focus on junction c
at that junction we have a current of three amps that is entering the junction
and 1.5 amps flows in this direction now according to kirchhoff's current law or his junction rule
the total current that enters into a junction is equal to the total current that leaves the junction
so if we call this i1 and this i2 then this must be i3
and so i1 enters the junction and the other two currents they leave it so i1 is equal to i2 plus i3
so i1 is 3 amps i2 is 1.5 so i3 is 3 minus 1.5 so this is also 1.5
amps so now we have the current flowing through the remaining three resistors
so i'm just going to put it here 1.5 amps now since the current flows from c to d
we know this is going to be positive and this is negative and it flows from d to e so
e is at a low potential then d and then it flows from e to f which means e is at a higher potential
than f now let's calculate the electric potential at point d
so the potential at point d is going to be the potential at point c minus ir
because as we go in the direction of the current we're going towards a lower potential
so d is lower than c the potential at c is 30. the current flowing through the 5 ohm
resistor is 1.5 so the voltage drop is 1.5 times 5 which is
7.5 and so 30 minus 7.5 tells us that the potential at d is
22.5 volts now let's calculate the potential at e so we have another voltage drop because
we're going towards a lower potential as we follow the direction of the current so it's going to be vd
minus ir so the potential at d is 22.5 we still have a current of 1.5 but this
time it goes to a 3 ohm resistor so 3 times 1.5 that's a voltage drop of 4.5
and 22.5 minus 4.5 gives us a potential of 18 volts at e
now to confirm the answer let's calculate the current going through the 2 ohm resistor
we already know it's 1.5 but let's confirm that answer because we have the potential at point f
so the potential at e minus the potential at f represents the voltage across the 2 ohm
resistor and voltage is equal to current times resistance
so the potential at e is 18 the potential f is 15 and r is 2.
so 18 minus 15 gives us a voltage of 3 volts and so 3 divided by 2
is 1.5 which is in agreement with this answer so now we've completely solved the
circuit we've calculated the current flowing through every resistor
and we also know the electric potential at every point in a circuit
and so that's it now if we wish to calculate the power absorbed by resistor
let's say if we want to calculate the power absorbed by this resistor we can use this formula i squared times
r so the current that's flowing through it is 1.5 and the resistance is 10. so the power absorbed by that resistor
is simply 22.5 watts now if we wish to calculate the power delivered by the battery
we can use this formula it's voltage times current so we have 60 volts
times the current of 3 amps and so that's going to be 180 watts now the power delivered by the battery
must be equal to the power absorbed by each resistor and that's the second way you can
confirm if you have the right answer so let's calculate the power absorbed by each resistor so we already have this
one and we said that's 22.5 watts
now let's focus on this resistor so it's i squared times r it's 3 squared times 10
and so the power absorbed by that resistor is 90 watts and for this one i squared times r is
going to be 3 squared times 5 and so it's 45 watts for that resistor and now for this one
it's going to be 1.5 squared times 5 and that's 11.25 and then for this one it's 1.5 squared
times 3. and so that's only 6.75 and then for this one 1.5 squared times
2 so that consumes 4.5 watts so now let's add up all the numbers
so we have 90 watts plus 45 plus 22.5
and then plus 11.25 plus 6.75 and then plus 4.5
let's see if that adds up to 180 and indeed it does so the total power absorbed by the
resistors is equal to the power delivered by the battery
and so this circuit the values that we have in this circuit is correct
now let's work on a similar circuit but one that's slightly different in a way
so we're just going to add one more resistor to the circuit that we had before
and the values will change of course so what if we put a resistor right in the middle
so this time we're going to have a 120 volt battery and this resistor is going to be 10 ohms
and this one is 12 ohms and this is going to be an 8 ohm
resistor and then 3 9
5 and in the middle this is going to be a 4 ohm resistor so feel free to pause the video
calculate the current that is delivered from the battery and the current that flows through each resistor in a circuit
so go ahead and try this problem now the first thing we need to do is calculate the equivalent
resistance so we need to know which resistors are in series and which ones
are parallel to each other now a series circuit is one in which the current has only one path to flow so
notice that the three and the nine ohm resistor they're in series with each other
because the current can't leave this junction so there's a single path of the currency
flow so we can replace those two with a 12 ohm resistor
so now the circuit becomes what we have here so this is still 10
8 and 12. and now i can write it like this
so i'm going to replace these two with a 12 ohm resistor and this is five
now we still have this resistor going in this direction now these two points are identical
so i can say that this resistor is going in this direction it's the same as drawing it this way
because they're attached to the same thing so this is four the 12 ohm resistor is
in parallel with the 4 ohm resistor now because these values are different
we're going to have to use a formula to find the equivalent resistance and
we can replace this 12 with the equivalent resistance so the equivalent resistance between
those two is going to be one over r one or one over four plus one over r two or one over twelve
raised to the minus one one fourth plus one twelve is one over three
if you use your calculator or if you like get common denominators
and then if you raise it to minus one it's three now if you don't have access to a
calculator here's what we need to do multiply this fraction by three over three
so it's going to be three over twelve plus one over twelve and three plus one is four to get four
over twelve and whenever you raise a fraction to the negative one power you need to flip the
fraction so it becomes twelve over four which is the same as three
so the equivalent resistance of those two in parallel is 3 ohms now notice that
the 3 ohm and the 5 ohm they're in series with each other there's only one path for the current to flow and three
plus five is eight so we can replace this with a eight ohm resistor
and that eight ohm resistor is in parallel with this eight ohm resistor and because
they're the same we know that the equivalent resistance of those two will be half
of the individual values so we can replace that with a 4 ohm resistor
so now the total resistance is going to be 10 plus 12 plus 4
which is 26 ohms so that's the equivalent resistance
now let's calculate the current in the circuit so it's going to be the voltage of the
battery divided by the equivalent resistance and so that's 120 volts
divided by 26 ohms and so the current that leaves the battery
is 4.615 amps and that's a rounded answer so keep that
in mind now let's define this point as point a
b c d e and f
and we're gonna assign point a a potential of zero volts so let's calculate the potential
everywhere else and at the same time let's calculate the currents and other positions
now going from b to c we know that the resistor i mean the potential decreases from high to low
because the current is flowing in that direction the current always flows from high potential to low
potential now the potential at b if we go from a to b we're going towards uh the positive
terminal of the battery so that's going to be a voltage lift of 120 so the potential at b
is 120 volts relative to a so now that we have the potential at b we can calculate the potential at c
and so it's going to be a voltage drop across this resistor so the potential at c is going to be the potential at b
minus ir so at b is 120 volts and the current flowing through the 10
ohm resistor is 4.615 multiplied by resistance of 10. so the potential at c
is 73.85 volts now let's go from a to f
so the current is flowing in this direction and that current is the same as this
current so this potential is positive and over here this side of the resistor
is negative so f is at a higher potential than a so the potential at f is going to be the
potential at a plus ir because as we go from a to f we're going towards the positive
terminal of the resistor towards the higher potential so a is zero the current is 4.615
and the resistance is 12. so 4.615 times 12 that will give us a potential of
55.38 volts at f now that we have the electric potential
at point c and f we can now calculate the current going through the 8 ohm resistor
now the current is going to be flowing in this direction so that it can reach the negative
terminal of the battery so therefore we know that this part of the resistor is positive
and this part is negative also we can see that c is at a higher potential than f so current always flows
from high potential to low potential so the potential at c minus the potential at f represents the voltage
across the 8 ohm resistor so remember voltage is the potential difference between two points
and that's equal to i times r so the electric potential at point c is 73.85 volts and that point f is
55.38 volts and the resistance is 8 ohms so 73.85
minus 55.38 that gives us a voltage of 18.47 so to calculate the current
it's going to be 18.47 divided by 8. so the current that flows through that resistor
let's see if i could fit it in here it's 2.309 if we round it
so i'm going to highlight that in red amps so
if we have a current of 4.615 going towards point c and a current of 2.309
amps going this way now the current that flows through this
branch and that branch has to be the difference between these two values
and because we have two different branches from c to d and c to
e we don't know what the answer is yet however there is something that we can
do so let's say if we have a picture that looks like this
so from c to e we know that this represents a resistance of 12 ohms it's three plus
nine and the current flowing through that branch is going to be the same
through the 3 ohm resistor and through the 9 ohm resistor so we're going to say this resistance is 12.
and the current that flows through this branch goes to a 4 ohm resistor now the current that is going towards
junction c which is right here over here this is a junction
e the current that flows to c is 4.615 amps
and the current that leaves that branch is 2.309 now the current that leaves junction c
to be split off into these two resistors that's going to be the difference of 4.615
and 2.309 and so that's going to be 2.306
that goes in that direction now notice how we're going to calculate the current that flows through each of
those two branches individually so let me just redraw this so right now we have a current
of 2.306 amps going in
so we'll call it it and this is a a 12 ohm resistor and this is a 4 ohm
resistor so with this information alone how can we calculate the current that flows
through the 12 ohm resistor and the current that flows through the 4 ohm resistor
now let's call the current that flows through the 12 ohm resistor i1 and the current that flows through the 4 ohm
resistor i2 we know that i1 plus i2 has to add up to the total current entering this little circuit
and notice that this resistance is less and this resistance is more so which
branch should have a greater current is i1 greater than i2 or is i2 greater than i1
now whenever you decrease the resistance the current increases so because this resistance is less than the other one
i2 is greater than i1 so because this is three times less than 12
i2 is going to be three times greater than i1 so we need two numbers
that add up to 2.306 and
we know that i2 has to be 3 times the value of i1 so we can replace i2 with 3i1
so it's i1 plus 3i1 and that's equal to 2.306 and so 4i1 is equal to that number
and 2.306 divided by 4 tells us that i1 is
0.5765 amps so to calculate i2 it's going to be 2.306
minus 0.5765 and so this current is 1.7295
as we can see this number is three times greater than that number
now it turns out that there's another way in which we can get the answer because sometimes these two resistors
may not be so nice you may have some other numbers that are just hard to work with
so let's call this r1 the 12 ohm resistor and this is r2 so let's say if we wish to calculate i1
it's going to be the total current times the other resistor r2 divided by the total resistance
so the total current entering this little circuit is 2.306 and r2
is 4. r1 plus r2 is 16. so it's 2.306 times 4 over 16 and that will give you 0.5765
now if you wish to calculate i2 you can use this equation
i2 is going to be the total current times the other resistor r1 divided by the total resistance r1 plus r2
so the total current is still 2.306 r1 is 12 r1 plus r2 is 16. so it becomes 2.306 times 12
divided by 16 and that will give you this current 1.7295 amps
so let's write this information here so we have the current flowing in this branch
that's through the 12 ohm resistor so that's 0.5 amps
we don't need this information anymore so let's just get rid of that
and we can get rid of this now the current flowing through the 4 ohm resistor
we said that's 0.5765 amps i should have made the circuit bigger
now let's calculate the potential at d so with the current is flowing through
the 3 ohm resistor in that direction so this has to be the positive terminal of the resistor and this is the negative
terminal of the resistor as it flows from c to d we know that d is a lower potential than the potential at c
so we can say that the potential at d is the potential at c minus i r
the electric potential at c is 73.85 and the current flowing through the 3 ohm resistor
we now know it to be 0.5765 so let's multiply that by 3. and so the potential at point d is
72.12 volts so now let's calculate the electric potential at e
so it's going to be the potential at e minus the potential at d
actually let's not do it that way the potential at e rather is the potential at d minus i r
we're still flowing in the direction of the current as we go from d to e so we still have a voltage drop across
this resistor so anytime we follow the direction of the current
if we move from d to e in the direction of the current that's going to be a voltage drop if we move from e to d
against the current that's a voltage lift so the potential at d we said it's 72.12
and the current is 0.5765 times the resistance of 9. and so the potential at e
is 66.93 volts now i need to correct this current
the current flowing through the 4 ohm resistor had to be the difference between
this current this one and that one so i believe it was like 1.7 something so if we take 4.615
subtract that by 2.309 and subtract that by 0.5765 this current was supposed to be 1.7295
amps now let's confirm this answer because we now have the electric potential between
c and e so we have the voltage across the 4 ohm resistor so current is going to flow from c to e
from high potential to low potential so vc minus ve that's going to be the
voltage across the 4 ohm resistor so vc is 73.85 the e
is 66.93 and that's gonna equal i times four so 73.85 minus 66.93
that's a voltage of 6.92 and divide that by 4 that will give us a current of 1.73 amps
which if you round it that's about the same as 1.7295 so we know that the numbers that we have
so far are correct now we have the potential at e and f so let's calculate the current that flows
from e to f so it's going to be v e minus v f and that's equal to i r so
the potential at e is 66.93 the potential at f is
55.38 and the resistance is 5. so 66.93 minus 55.38
that gives us a voltage of 11.55 so if we divide that by 5
then the current flowing through the 5 ohm resistor is 2.31 amps to confirm this answer
notice that the current that flows from d to e and the current that flows from c to e
must equal the current that flows from e to f which is this current so if we add 0.5765
plus 1.7295 that gives us a current of 2.306
which if you round it that's approximately 2.31 so we have confirmed every value in the
circuit so all the potentials and the currents flowing through each resistor that you
see is correct now we can calculate the power absorbed by each resistor and the power delivered
by the battery but you know how to do that at this point so you can check it that way as well
the power delivered by the battery has to equal to the total power absorbed by all of the resistors
and that could be the final check if you want to make sure your work is correct so that's it for this video
and now you know how to solve any type of series parallel combination circuit
where you have one battery and just a bunch of resistors so thanks again for watching
you
To identify series resistors, look for components connected end-to-end, where the same current flows sequentially through each resistor. Parallel resistors share both connection nodes directly, meaning they have the same voltage across them. Breaking down the circuit by labeling nodes helps to spot these groupings clearly for step-by-step simplification.
Start by identifying and combining all series resistors by simply adding their resistances. Next, simplify parallel resistor groups using the formula 1/R_eq=1/R1+1/R2+..., or halve the resistance if they are equal-valued. Repeat this gradual simplification until the entire circuit reduces to a single equivalent resistance.
First, calculate the total current from the battery using Ohm's Law (I_total = V_battery / R_eq). Then, at junctions, apply Kirchhoff's Current Law to ensure current splitting balances. Use the current division rule: I_branch = I_total × (R_other / (R_branch + R_other)) for two parallel branches, or use voltage differences and Ohm's Law (I = V / R) if node potentials are known.
Choose a reference node and assign it 0 volts (often the negative terminal of the battery). Follow the current direction and add the battery voltage when moving from negative to positive terminals. Calculate potentials at other nodes by subtracting or adding voltage drops (V = I × R), considering the direction of current flow through each resistor.
Calculate the power absorbed by each resistor using P = I^2 × R and sum all these values. Then, calculate the power delivered by the battery with P = V × I_total. If both sums match closely, it confirms that your voltage, current, and resistance calculations are consistent and accurate.
Label all nodes clearly and assign a reference potential early. Break the circuit into simpler series and parallel sections for easier analysis. Carefully track voltage rises and drops following the direction of current flow. Use Kirchhoff’s Current Law at junctions for current splitting and always verify your answers with power balance calculations.
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