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TRANSCRIPT
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INSTITUTO POLITCNICO NACIONALESCUELA SUPERIOR DE COMPUTO
Node AnalysisFundamental Analysis of Circuits Laboratory
Arceta Torres Fernando
Pazarn Rodrguez Samy Zabdiel
Urquiza Lpez Carlos Ariad
Mexico D. F. 23 of October of 2012
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INSTITUTO POLITCNICO NACIONAL
Escuela Superior de Cmputo
Fundamental Analysis of Circuits Laboratory
Practice 5: Node Analysis
Target:
The student applied the method to determine the voltage nodes present in an electrical circuit, sothat at the end of practice, this in a position to employ this technique in calculating the voltage
drop present in networks that contain multiple nodes.
Equip provided by Laboratory:
1 Digital Multimeter
1 Variable Voltage sources CD
4 Banana-alligator connectors
4 Banana-Banana connectors Cutting pliers
Nose pliers
Material owned by students: 1 Protoboard
2 Resistors of 680 .
2 Resistors of 330 .
1 Resistors of 270 .
1 Resistors of 560 .
1 Resistors of 100 .
2 Resistors of 1 k ..
Connection cables for Breadboard.
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I Theoretical Introduction
In electric circuits analysis, nodal analysis, node-voltage analysis, or the branch current
method is a method of determining the voltage (potential difference) between "nodes"
(points where elements or branches connect) in an electrical circuit in terms of the branch
currents.
In analyzing a circuit using Kirchhoff's circuit laws, one can either do nodal
analysis using Kirchhoff's current law (KCL) or mesh analysis using
Kirchhoff's voltage law (KVL). Nodal analysis writes an equation at each
electrical node, requiring that the branch currents incident at a node must
sum to zero. The branch currents are written in terms of the circuit node
voltages. As a consequence, each branch constitutive relation must give
current as a function of voltage; an admittance representation. For
instance, for a resistor, Ibranch = Vbranch * G, where G (=1/R) is the
admittance (conductance) of the resistor.
Nodal analysis is possible when all the circuit elements' branch constitutive
relations have an admittance representation. Nodal analysis produces a compact set of
equations for the network, which can be solved by hand if small, or can be quickly solved
using linear algebra by computer. Because of the compact system of equations, many
circuit simulation programs use nodal analysis as a basis. When elements do not have
admittance representations, a more general extension of nodal analysis, modified nodal
analysis, can be used.
Method:
1. Note all connected wire segments in the circuit. These are the nodes of nodal
analysis.
2. Select one node as the ground reference. The choice does not affect the result and is
just a matter of convention. Choosing the node with most connections can simplify the
analysis.
3. Assign a variable for each node whose voltage is unknown. If the voltage is already
known, it is not necessary to assign a variable.
4. For each unknown voltage, form an equation based on Kirchhoff's current law.
Basically, add together all currents leaving from the node and mark the sum equal to zero.
5. If there are voltage sources between two unknown voltages, join the two nodes as a
supernode. The currents of the two nodes are combined in a single equation, and a new
equation for the voltages is formed.
6. Solve the system of simultaneous equations for each unknown voltage.
Kirchhoff's current law
is the basis of nodal
analysis.
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II Practice Development
II.1 Applying the method of circuit nodes to the figure, find a theoretical way (analytical
method), the corresponding current values called for in certain items and list them on the
table.
II.2 Without turning the voltage source, build the circuit, on the protoboard. Once armed,
proceed to set the voltage value indicated and applied to the circuit through the probes, the
power supply on.
II.3 Check the validity of previous theoretical results by measuring with the ammeter, the
current in the above points and report their practical values of the table.
MeasurementsTheoretical value
(ampers)Measured value (ampers)
Current I - 0 4.92 A 4.90 A
Current II - I 2.31 A 2.32 A
Current II - 0 2.75 A 2.75 A
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II.4 The same circuit voltage obtained theoretical values obtained in the simulator and
experimental, report them in the following table.
MeasurementsTheoretical value
(volts) Measured value (volts)
Voltage V I 0 3.81 V rms 3.6 V rms
Voltage V II 0 600 mV rms 550 mV rms
Voltage V I II 3.22 V rms 3.04 V rms
II.5 Finally calculate the power dissipated by each resistor and record in the table.
Resistors (K)power dissipated
(watts)
R1 12.9 mW
R2 3.02 mW
R3 77 mW
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III.- Questionary
1. Define what is a node in an electrical circuit.
In an electrical circuit connection points of three or more drivers which we callnodes or knots. Half point or a field that remains unchanged when more than one
disturbance simultaneously acting on it.
2. Define what is the voltage of a node.
In a series circuit the sum of the potential difference across each element ofconsumption hereinafter called voltage drop is equal to the voltage that providesthe power source or battery.
3. What we call the reference node?
The reference node is chosen arbitrarily, although it is common to choose the nodewhich is connected to a larger number of branches or a node with a voltagesource. In most cases, this procedure involves a smaller number of equations.
4. Briefly define the method that consists of nodes.
It is a general method of circuit analysis is based on determining the voltages of allcircuit nodes with respect to a reference node. Known these voltages candetermine all the currents in the various circuit elements.
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IV.- Conclusions
Arceta Torres Fernando
In developing this practice we saw the issue of analysis of nodes seen in class, which this
method is much easier to me than the Kirchoff current law.
Pazarn Rodrguez Samy Zabdiel
This practice could apply and verify knowledge previously obtained theoretical classes on
the use of the method of Node Analysis for the calculation of voltages and currents in a
circuit of four meshes with current sources later gaining power in each of the nine
resistance existed.
Urquiza Lpez Carlos Ariad
In this practice we could see the reasoning of the Node Analysis by circuit simulation, and
by calculating the equations for the node.
The use of the law is very useful for resuloucion in cases that include current sources in
the mesh.