Nodal Analysis EP.16 (Tagalog/English Electronics)
Summary
TLDRThis video script is a tutorial on nodal analysis, a method for analyzing electrical circuits. It guides viewers through selecting a reference node, assigning voltages to other nodes, and applying Kirchhoff's Current Law to derive equations. The tutorial uses Ohm's Law to express branch currents in terms of node voltages and demonstrates solving simultaneous equations to find unknown voltages. An example circuit is used to illustrate the process, showing calculations for node voltages and currents through resistors.
Takeaways
- ๐ Nodal analysis is a method for analyzing electrical circuits by considering the voltages at various nodes.
- ๐ง The first step in nodal analysis is to select a reference node and assign voltages to the remaining nodes.
- ๐ Kirchhoff's Current Law (KCL) is applied to each node to set up equations relating the node voltages.
- โ๏ธ Ohm's Law is used to express branch currents in terms of node voltages and resistance.
- ๐งฎ Solving the simultaneous equations obtained from the KCL and Ohm's Law applications yields the unknown node voltages.
- ๐ Nodal analysis is particularly useful for circuits with multiple nodes and complex interactions.
- ๐ก The reference node is often grounded to simplify calculations, making it a common point of reference.
- ๐ Current directions are assigned for each node, and the currents entering and leaving a node are balanced according to KCL.
- ๐ The script provides a step-by-step example of applying nodal analysis to a circuit with a voltage source and resistors.
- ๐ ๏ธ The solution involves calculating currents through resistors and voltages across nodes using the derived nodal equations.
Q & A
What is nodal analysis in electrical circuits?
-Nodal analysis is a method used to analyze electrical circuits by considering the voltages at different nodes and applying Kirchhoff's Current Law (KCL) to derive equations that can be solved to find the unknown node voltages.
Why is selecting a reference node important in nodal analysis?
-Selecting a reference node, typically grounded, is crucial because it provides a common point of reference for measuring the voltages at other nodes in the circuit, simplifying the formulation of nodal equations.
How do you assign voltages to nodes in nodal analysis?
-In nodal analysis, you assign voltages (v1, v2, ..., v(n-1)) to the remaining nodes after selecting a reference node. The reference node is often assigned a voltage of zero.
What is the role of Ohm's Law in nodal analysis?
-Ohm's Law is used in nodal analysis to express the branch currents in terms of node voltages by relating the voltage across a resistor to the current through it (V = IR), which helps in formulating the nodal equations.
How many nodal equations are typically formed in a nodal analysis?
-The number of nodal equations formed is typically one less than the number of nodes (N-1), where N is the total number of nodes in the circuit.
What is the significance of Kirchhoff's Current Law (KCL) in nodal analysis?
-KCL is essential in nodal analysis as it states that the sum of currents entering a node is equal to the sum of currents leaving that node, which is used to set up the equations for each node.
Can you explain how to solve the simultaneous equations obtained from nodal analysis?
-The simultaneous equations from nodal analysis can be solved using algebraic methods like Cramer's rule, or numerical methods using software like MATLAB. The goal is to find the unknown node voltages.
What is the purpose of assigning currents in the direction of voltage drops in nodal analysis?
-Assigning currents in the direction of voltage drops helps in determining the sign of the current terms when formulating the nodal equations, which is necessary for accurately representing the flow of current in the circuit.
How does the choice of the reference node affect the nodal analysis?
-The choice of the reference node does not affect the solution of the nodal analysis but simplifies the process by reducing the number of unknowns and making the equations easier to set up and solve.
What are the common techniques used to solve the equations resulting from nodal analysis?
-Common techniques to solve the equations from nodal analysis include Cramer's rule for small systems, matrix methods for larger systems, and numerical methods or software tools like MATLAB for complex circuits.
Outlines
๐ Introduction to Nodal Analysis
The paragraph introduces the concept of nodal analysis in electrical circuit analysis. It explains that nodal analysis involves applying Kirchhoff's Current Law (KCL) at each node in a circuit, excluding the reference node. The process involves selecting a reference node, assigning voltages to the remaining nodes, and setting up equations based on the currents entering and leaving each node. The summary also mentions the use of Ohm's law to express branch currents in terms of node voltages and the solving of simultaneous equations to find the unknown voltages.
๐ Applying Nodal Analysis to a Sample Circuit
This paragraph delves into applying nodal analysis to a specific example circuit. It describes the process of selecting a reference node, assigning voltages to other nodes, and setting up KCL equations. The summary explains how to use Ohm's law to express currents in terms of voltages and resistances, and how to solve the equations to find node voltages. It also mentions the common practice of grounding the reference node to simplify calculations.
๐งฎ Solving Nodal Equations
The paragraph focuses on solving the nodal equations derived from the circuit analysis. It discusses the process of combining equations and simplifying them to isolate node voltages. The summary includes the use of algebraic techniques and tools like MATLAB to solve simultaneous equations. It also provides a step-by-step explanation of how to manipulate equations to find the node voltages in the example circuit.
๐ Detailed Calculations and Voltage Determination
This paragraph provides a detailed account of the calculations involved in determining node voltages. It explains the process of substituting values into the nodal equations and solving for the unknowns. The summary includes specific numerical values and the steps taken to arrive at the node voltages, including the use of voltage division across resistors and current direction.
๐ Conclusion of Nodal Analysis Example
The final paragraph wraps up the nodal analysis example by summarizing the findings and the process. It confirms the node voltages obtained from the calculations and reiterates the steps involved in the analysis. The summary also mentions the verification of the results by checking the current through resistors and the voltage across them, ensuring the analysis is consistent with the circuit's behavior.
Mindmap
Keywords
๐กNodal Analysis
๐กReference Node
๐กKirchhoff's Current Law (KCL)
๐กNode Voltages
๐กOhm's Law
๐กSimultaneous Equations
๐กCircuit Analysis
๐กResistors
๐กVoltage Source
๐กCurrent Source
๐กAlgebraic Techniques
Highlights
Introduction to nodal analysis as a method for electrical circuit analysis.
Explanation of the concept of nodal analysis, focusing on nodes in a circuit.
Selection of a reference node as the first step in nodal analysis.
Assignment of voltages to the remaining nodes with respect to the reference node.
Application of Kirchhoff's Current Law (KCL) to derive equations for the nodes.
Use of Ohm's Law to express branch currents in terms of node voltages.
Formation of simultaneous equations to solve for unknown node voltages.
Techniques for solving simultaneous equations, including algebraic methods and software tools.
Example problem walkthrough using nodal analysis to find node voltages.
Step-by-step approach to applying KCL and Ohm's Law to a given circuit.
Calculation of branch currents and their directions in the circuit.
Derivation of nodal equations for a specific node considering current sources and resistors.
Simplification of nodal equations to find relationships between node voltages.
Substitution of derived expressions into the nodal equations to solve for node voltages.
Use of a calculator to solve the system of equations for node voltages.
Verification of the calculated node voltages by back-substituting into the nodal equations.
Final results of the node voltages obtained through nodal analysis.
Conclusion of the nodal analysis tutorial with a summary of the process.
Transcripts
hi guys welcome engineer my channel
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analysis so amusing intimate opponent
just keep on watching so honorable nodal
analysis so basically our model analysis
is a Samana useful electrical circuit
analysis Chui Nagina gamut our Mesabi on
node voltage now some given circuit so
from the word itself nodal analysis the
consider not any embowered nodes say I
sound circuit and then again I got
nothing load ito yung Kirchhoff's
current law so Bobo Italian of equation
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circuit make up once either not n so
let's proceed in similar steps no bug at
i/o max of is an example using nodal
analysis okay so the first step is
select a node as the reference node
assign voltages v1 v2 and until V sub n
minus 1 to the remaining n minus 1 nodes
the voltage our reference with respect
to the reference node of a Suboxone
Abimelech tottenham a reference node
denotes a circuit na hindi not n Kohanim
KCl equations so basically commando tie
on that long nodes young Insadong
a gagarina the reference node and then
young adder to Union tokoha an addendum
KCl equation so burl a common contact
long nodes Valley NY 3 so minus 1 Mo
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Mona Cassell equations convert an N
nodes and - wanama boo-boo Amada patna
equations usually you in appealing
reference node a young ground as a zero
Xiao Yan you know first step ok select
manettino reference node and then Mikasa
internal node named Ansari meaning no
since a circuit our next step apply kcl
to each of the N minus 1 and reference
notes use Ohm's law to express the
branch currents in terms of node
voltages so in Alana not after not in my
determine new reference node at
mcconnell and young other node voltages
in a circuit a plane anata no KCl Danza
ballad note meaning sum of currents
entering a specific node is equal to sum
of currents leaving that specific node
and then come back in terms of current
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current ICO convert NAT and in terms of
voltage and resistance using Ohm's law
so McGee King V over R u colobus an
equation atom in terms of voltage
inertia okay and then the third step
solve the resulting simultaneous
equations to obtain the unknown voltage
so you know so Donna Mahabharata and n
minus 1 equations phenomena 10 is so
beyond using techniques in algebra like
reading Kramer's rule superboring
comma metonym MATLAB or in Patna Lynott
indirect Lisa algebra safe alkyl
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old nan Hangang 3 simultaneous equations
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turned on by the input u s-- about you
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three simultaneous equations in terms of
the node voltages
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some example param and straighten
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circuit Tito I think the training is
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voltage across the resistor as well as
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analysis so let's determine first
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notes valid neva Kohanim TCL equations I
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equations nada but in terms of the node
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the savvy one sermon on ginagawa ho I
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no consider can resist or within a
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equation 110 now i'm simply find an
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over it is 8 right plus V 1 over 4 minus
V 2 over 4 plus 2 is equal to 0 then
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over it's a positive V 1 over 4 so we
have V 1 1 8 plus 1 for the network V 2
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Athenian constant na+ to jihad negative
8 desire right sides a McGee negative 2
plus 8 so simplify naught into 1 8 plus
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plus 8 which is 6 away so this noise our
equation 1 now apply the final a VA na
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have become
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nothing so this is i2 and this time
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have a three and then you know um
currents are still nothing bad Bakugan
so this type of antenna Manchus ah no
two wakes up Lena ten so animal lamella
bus at an eye on I - so I'm higher
potentially I am V - no volume v1 so
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current is equal to 0 at t to Sosa I to
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say to Paula Amana live in LA + yawns r3
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the non lower potential Nia a young
reference node na ground which is equal
to 0 long so therefore we have V 2 minus
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voltage and Ewa and then equals as
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minus V 1 over R 2 is 4 ohm plus V 2
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now on combine that and similar terms
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plus V 2 over 10 is equal to 2 so
meringue negative V 1 over 4 plus V 2
times 1 4 + 1 10 is equal to 2 so
simplify nothing negative 1 4 is
negative 0.25 V 1 plus 1/4 plus 1/10 is
0.35 V 2 is equal to 2
the equation tuna tent so I would iron
on the low one equation from Equation
one Chaka equation to my own angle
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v1 v2 chairman are constants Neela
admission so no no Malcolm directly
volume v1 chaja v2 a singer hangang
three simultaneous equations champion in
Seoul also this time that have two
simultaneous equations tournament REO
material nothing is optimal Omanis of
apathetic on Ellen signor Contino Vaako
c-note cool equation 1 / v1 in terms of
v2 so it a on and then a substitute
reliant on v1 in terms of v2 the
circulation to Sam McGee negative 0.25
in v1 8006 plus 0.25 v2 over 0.375 okay
plus kappa nitendo remaining expressions
0.35 v2 is equal to 2 right on the hill
in terms of beaten along co-parent and
adding some muscle so if ship silcoon an
officer Arkell eternal pyramidal a so we
have v2 is equal to thirty two point
seventy three volts awaiting beaten
attend and then Paramahamsa v1 gave it
in a tent on equation a 10-6 plus 0.25
v2 i thirty two point seventy three
volts na over 0.375 oh my gammit
inordinate and your calculus of nothing
cv 1 which is equal to 37
point eighty two volts so in participate
you put the harasser mode five ten
billion a young one
okay then turn cell number one role
again numerical coefficients no v1 v2 to
a constant and say equation 1 so 0.375
equals negative 0.25 equals then six oh
hi didn't sorrow number two input
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v1b touch upon constant so I get the
observer point 25 equals 0.35 equals and
then two and then press equal sign
submissively
X or you know V 1 so value in your eye
thirty-seven point eighty one so packed
Vanessa Minnillo
equal Assad Miriam why a union B to some
file in your eye thirty two point seven
two seven okay so not gonna happen
you'll not be one happy to play on put
in an attic muscle embark on don't see
resistors r1 r2 chaja our tree so Hanina
sa diba and representation attended
seminar that says r1 at all young I 1 is
equals v1 minus 64 volt over it right so
by the way whom are lagging value not
infer current I negative come as a
substitute not a new number one adding
node voltages the city was a v1 minus 64
over a double monitoring v1 specs
innovated not a new v1 NACA Honiton
kanina minus 64 over it at the resulting
current i- Avelina yep except in
london's
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debenture a national ana paula lucia p1
so home- Mannschaft
the pad Paula are McGee
I pop on the savvy one castle- young
valladon Akhenaton so condiment
compositive nominee B sub n tamanna oven
nothing current so let's try to check
okay so the RI 1 is equal to V 1 minus
64 over it right okay so V 1 at and
Anaka by thirty seven point eighty two
volts minus 64 volts over eight so else
I got i- 3.27 amps so Tahu negative yep
exhibition long-known young current i1
and direction need a path not kunai eye
upon Tasha node v1 pero same magnitude
Purina 3.27 okay so i1 is poppin Tasha
v1 and then your voltage shouldn't say
r1 which is p2 equal measure Danza the
above v1 minus 64 since negative boom
knock over nothing current veto it
because I've been long known 64 minus v1
Shah so therefore we have 64-37 point
ATP which is equal to twenty six point
eight bean pods
okay so banana tech nothing new what
exciting as a belief that I am Karan
so para Mac positively on Baltic Sonya
share ever - nothing lower voltage w1
Danza higher voltage Tina 64 okay now
determines
r2 so this time Sartain upon single
delivering initial nothing flows no
currently back on with respects of v1
unlocking direction no current nuttin
a-poppin tahan and convert the spectrum
and savvy to preferred animal Sakawa so
my own appellate nothing in general
consequence and direction chammak
positive value of Chaeronea union taman
direction yeah so termina not
incompetent Asahara and so
representation not in a v1 minus v2 over
FERPA
the back so let's try so I 2 is equal to
V 1 minus V 2 over 4 so V 1 is 37.8 e 2
volts minus V 2 is 32 point seven three
volts over four so therefore i2 is equal
to positive one point twenty seven amps
so therefore tamo
in direction and Hashem natin sa
positive nominee Canela bassam value new
current okay so I'm directional I 2 is
began on okay and then your voltage
across r2 now is same perineum v1 minus
v2 Isetta Menomonee on nagging direction
at the national aren t so 3/2 is v1
minus v2 or thirty-seven point eighty
two volts minus thirty-two point seven
three watts which is equal to five point
zero nine points okay and then dunam
answer are three we have an assumed not
an i V 2 minus zero right so part of v2
over r3 so try not uncommon per positive
value no Erin
so I 3 is v2 over r3 so since positive
nominal node voltage V donut and some a
capacitive Naga diem current so v2 is
thirty two point seventy three volts
over R three witches ten humps so
therefore I three is three point two
seven three amps
okay so Tamayo direction at a no
carranza are three SOPA Basia
and then you voltage across R 3 which is
that say V three equations a veto right
as a v2 minus zero element or v2 which
is equal to
thirty two point seventy three volts
okay
cigar normal analyzed non circuit using
nodal analysis okay
mnemonic on challenge signal I have a
given circuit which is the circuit and
then find the node voltages v1 and v2
using nodal analysis so Ana Pinero to v1
to v2 using nodal analysis by forming
KCl equation stencil node v1 to v2
since the lava Melanie not nananana na
Dhin calomel an and the lava KCl
equations and two equations in two
unknowns so model edentia okay so that's
it for the nodal analysis topics so sana
ma NATO Dolan chaos aficionado at
maraming salamat happenin hood
[Music]
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