1.1 KIRCHOFF’S LAWS
• Kirchoff’s Current Law: “The sum of currents at any node in a circuit must equal zero” - keep in mind that current is a flow rate for moving electrons. And, electrons do not appear and disappear from the circuit. Therefore, all of the electrons flowing into a point in the circuit must be flowing back out.
• Kirchoff’s Voltage Law: “The sum of all voltages about a closed loop in a circuit is equal to zero” - Each element will have a voltage (potential) between nodes. If any two points on the closed loop are chosen, and different paths chosen between them, the potentials must be equal or current will flow in a loop indefinately (Note: this would be perpetual motion).
1.1.1 Simple Applications of Kirchoff’s Laws
184.108.40.206 - Parallel Resistors
• Let’s consider one on the most common electrical calculations - that for resistors in parallel. We want to find the equivalent resistance for the network of resistors shown.
220.127.116.11 - Series Resistors
• Now consider another problem with series resistors. We can use Kirchoff’s voltage law to sum the voltages in the circuit loop. In this case the input voltage is a voltage rise, and the resistors are voltage drops (the signs will be opposite).
1.1.2 Node Voltage Methods
• If we consider that each conductor in a circuit has a voltage level, and that the components act as bridges between these, then we can try some calculations.
• This method basically involves setting variables, and then doing a lot of algebra.
• This is a very direct implementation of Kirchoff’s current law.
• First, let’s consider an application of The Node Voltage method for the circuit given below,
1.1.3 Current Mesh Methods
• If we consider Kirchoff’s Voltage law, we could look at any circuit as a collection of current loops. In some cases these current loops pass through the same components.
• We can define a loop (mesh) current for each clear loop in a circuit diagram. Each of these can be given a variable name, and equations can be written for each loop current.
• These methods are quite well suited to matrix solutions
• Lets consider a simple problem,
1.1.4 More Advanced Applications
18.104.22.168 - Voltage Dividers
• The voltage divider is a very common and useful circuit configuration. Consider the circuit below, we add a current loop, and assume there is no current out at Vo,
22.214.171.124 - The Wheatstone Bridge
• The wheatstone bridge is a very common engineering tool for magnifying and measuring signals. In this circuit a supply voltage Vs is used to power the circuit. Resistors R1 and R2 are generally equal, Rx is a resistance to be measured, and R3 is a tuning resistor. An ammeter is shown in the center, and resistor R3 is varied until the current in the center Ig is zero.
126.96.36.199 - Tee-To-Pi (Y to Delta) Conversion
• It is fairly common to use a model of a circuit. This model can then be transformed or modified as required.
• A very common model and conversion is the Tee to Pi conversion in electronics. A similar conversion is done for power circuits called delta to y.
• We can find equivalent resistors considering that,
• To find the equivalents the other way,
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