Opening Kirchoff!
... Calculate the result using 1kΩ resistors: R3 ll R4 : 1/1kΩ + 1/1kΩ = 1/R = 2/1kΩ or R = 0.5 kΩ R + R5 = 1.5 kΩ R2 ll 1.5 kΩ = 1/1kΩ + 1/1.5kΩ = 5 / 3kΩ so R = 0.6kΩ R1 + 0.6kΩ = 1.6kΩ = Rtot 10V = Itot Rtot = Itot (1.6kΩ) Itot = 10V / Rtot = 10V / 1.6kΩ = 6.25mA same as before. The rest follows from ...
... Calculate the result using 1kΩ resistors: R3 ll R4 : 1/1kΩ + 1/1kΩ = 1/R = 2/1kΩ or R = 0.5 kΩ R + R5 = 1.5 kΩ R2 ll 1.5 kΩ = 1/1kΩ + 1/1.5kΩ = 5 / 3kΩ so R = 0.6kΩ R1 + 0.6kΩ = 1.6kΩ = Rtot 10V = Itot Rtot = Itot (1.6kΩ) Itot = 10V / Rtot = 10V / 1.6kΩ = 6.25mA same as before. The rest follows from ...
Syllabus - Jongwon Lee
... prohibited and will be appropriately punished. When preparing homework you are allowed to discuss with other peer students, but all material submitted must be original. Notes on exam grading: For exam problems, reasoning and analysis are typically as or more important than the final answer. You shou ...
... prohibited and will be appropriately punished. When preparing homework you are allowed to discuss with other peer students, but all material submitted must be original. Notes on exam grading: For exam problems, reasoning and analysis are typically as or more important than the final answer. You shou ...
File
... • Every circuit has n nodes with one of the nodes being designated as a reference node • We designate the remaining n – 1 nodes as voltage nodes and give each node a unique name, vi. • At each node we write Kirchhoff’s current law in terms of the node voltages • We form n-1 linear equations at the n ...
... • Every circuit has n nodes with one of the nodes being designated as a reference node • We designate the remaining n – 1 nodes as voltage nodes and give each node a unique name, vi. • At each node we write Kirchhoff’s current law in terms of the node voltages • We form n-1 linear equations at the n ...
This is what the circuit looked like as I was setting it up
... hand by adding all the voltages in a loop that the total is always equal to zero, which is in accordance with Kirchhoff’s Voltage Law. Included in the objective was applying our knowledge of how to use a bread board and how to create a circuit with two separate voltage sources. Another objective of ...
... hand by adding all the voltages in a loop that the total is always equal to zero, which is in accordance with Kirchhoff’s Voltage Law. Included in the objective was applying our knowledge of how to use a bread board and how to create a circuit with two separate voltage sources. Another objective of ...
Transient Analysis of Electrical Circuits Using Runge
... consisting of a resistor, an inductor, and a capacitor, connected in series or in parallel. The RLC part of the name is due to those letters being the usual electrical symbols for resistance, inductance and capacitance respectively. The circuit forms a harmonic oscillator for current and will resona ...
... consisting of a resistor, an inductor, and a capacitor, connected in series or in parallel. The RLC part of the name is due to those letters being the usual electrical symbols for resistance, inductance and capacitance respectively. The circuit forms a harmonic oscillator for current and will resona ...
Chapter 8 – Methods of Analysis and Selected Topics (dc)
... negative sign if it draws current from the node. 5. Solve the resulting simultaneous equations for the desired voltages. ...
... negative sign if it draws current from the node. 5. Solve the resulting simultaneous equations for the desired voltages. ...
Variable Resistors - School
... As the water cools, the resistance rises and results should be recorded at regular intervals of temperature. ...
... As the water cools, the resistance rises and results should be recorded at regular intervals of temperature. ...
LectNotes4-MeshAnalysis
... (Sort of like the branch voltage of a branch connected to the reference node.) Now write KVL around the loop defined by each mesh, in terms of mesh currents. Remember how in nodal analysis we used current leaving a node, even though KCL is stated in terms of current entering a node? Well, now we'll ...
... (Sort of like the branch voltage of a branch connected to the reference node.) Now write KVL around the loop defined by each mesh, in terms of mesh currents. Remember how in nodal analysis we used current leaving a node, even though KCL is stated in terms of current entering a node? Well, now we'll ...
Installing Cabling: Procedures
... network, carry out pre-installation tests over a suitable period to access the full building characteristics over all times of day and days of the week. For domestic installations, it may be unnecessary to perform a pre-installation check. Node Count and Distribution With power line networks it is v ...
... network, carry out pre-installation tests over a suitable period to access the full building characteristics over all times of day and days of the week. For domestic installations, it may be unnecessary to perform a pre-installation check. Node Count and Distribution With power line networks it is v ...
Superposition
... independent sources in the original circuit. 7. To find the total voltage across each component and the total current flowing, add the contributions from each of the voltages and currents found in Step 3. ...
... independent sources in the original circuit. 7. To find the total voltage across each component and the total current flowing, add the contributions from each of the voltages and currents found in Step 3. ...
Module 1_Basic Electrical Concepts
... leaving the node must be assigned opposite algebraic signs . • Kirchhoff’s Voltage Law (KVL): It states that in a closed circuit, the algebraic sum of all source voltages must be equal to the algebraic sum of all the voltage drops. • Voltage drop is encountered when current flows in an element (resi ...
... leaving the node must be assigned opposite algebraic signs . • Kirchhoff’s Voltage Law (KVL): It states that in a closed circuit, the algebraic sum of all source voltages must be equal to the algebraic sum of all the voltage drops. • Voltage drop is encountered when current flows in an element (resi ...
Lecture 1-4 Summary file
... Inductance is measured in Henry (H). The relationship between voltage and current is given by n = N. dφ/dt = L. di/dt L = (N2μA)/l for a coil; where μ is the permeability, N the number of turns, l the length and A cross section of core. Energy stored in an inductor = ½ L i2 No energy is dissipated i ...
... Inductance is measured in Henry (H). The relationship between voltage and current is given by n = N. dφ/dt = L. di/dt L = (N2μA)/l for a coil; where μ is the permeability, N the number of turns, l the length and A cross section of core. Energy stored in an inductor = ½ L i2 No energy is dissipated i ...
Ch. 10
... • The same rules apply: Convert to frequency domain first, then apply KVL as usual. • In KVL, supermesh analysis is also valid. ...
... • The same rules apply: Convert to frequency domain first, then apply KVL as usual. • In KVL, supermesh analysis is also valid. ...
Lecture 7 Slides - Digilent Learn site
... Nodal Analysis – checking results • Checking results in step 5: • In general, in the equation for node “X”, the multiplicative factor on the node voltage VX will be the sum of the conductances at node “X” • The multiplicative factors on all other node voltages in the equation will be the negative o ...
... Nodal Analysis – checking results • Checking results in step 5: • In general, in the equation for node “X”, the multiplicative factor on the node voltage VX will be the sum of the conductances at node “X” • The multiplicative factors on all other node voltages in the equation will be the negative o ...
Topology (electrical circuits)
The topology of an electronic circuit is the form taken by the network of interconnections of the circuit components. Different specific values or ratings of the components are regarded as being the same topology. Topology is not concerned with the physical layout of components in a circuit, nor with their positions on a circuit diagram. It is only concerned with what connections exist between the components. There may be numerous physical layouts and circuit diagrams that all amount to the same topology.Strictly speaking, replacing a component with one of an entirely different type is still the same topology. In some contexts, however, these can loosely be described as different topologies. For instance, interchanging inductors and capacitors in a low-pass filter results in a high-pass filter. These might be described as high-pass and low-pass topologies even though the network topology is identical. A more correct term for these classes of object (that is, a network where the type of component is specified but not the absolute value) is prototype network.Electronic network topology is related to mathematical topology, in particular, for networks which contain only two-terminal devices, circuit topology can be viewed as an application of graph theory. In a network analysis of such a circuit from a topological point of view, the network nodes are the vertices of graph theory and the network branches are the edges of graph theory.Standard graph theory can be extended to deal with active components and multi-terminal devices such as integrated circuits. Graphs can also be used in the analysis of infinite networks.