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Sample of the Study Material Part of Chapter – 1 Network Methodology Network Theory Network Methodology SAMPLE OF THE STUDY MATERIAL PART OF CHAPTER – 1 NETWORK METHODOLOGY 1.1. Passive Components A passive component, depending on field, may be either a component that consumes (but does not produce) energy or a component that is incapable of power gain . The passive circuit elements resistance R, inductance L and capacitance C are defined by the manner in which voltage and current are related for the individual element. The table below summarizes the voltage-current (V-I) relation, instantaneous power (P) consumption and energy stored in the period [t, t] for each of above elements . The electrical resistance of an electrical element measures its opposition to the passage of an electric current; the inverse quantity is called conductance. The resistance of an object is defined as the ratio of voltage across it to current through it: = Inductance is the property of an electrical circuit causing voltage to be generated proportional to the rate of change in current in a circuit. Inductance is caused by the magnetic field generated by electric currents according to Ampere's law. Capacitance is the ability of a body to hold an electrical charge. Physically, a capacitor is two electrical conductors separated by a non-conducting (or very high resistance) medium between the conductors. Page : 1 Network Theory Network Methodology Table 1.1.Voltage –Current relation of network elements SL. Circuit Symbol in Units Voltage – Instantaneous Energy No element electric circuit current power , P stored / relation dissipated in [, ] 1 Resistance, R + V= i R (t − t) i Ohm ( ohm’s law) Vi= iR V ( ) − 2 Inductance, L i + Henry V = L Li 1 ( − ) V ( H ) 2 − 3 Capacitance, C i + Farad 1 i = C C ( − ) V ( F ) 2 − In the above table, if i is the current at instant m and V is the voltage at instant m, total energy dissipated in a resistor (R) in [ t, t ] =∫ v. i dt = ∫ i R dt Page : 2 Network Theory Network Methodology 1.2. Series and parallel connection of circuit elements Figure below summarizes equivalent resistance /inductance /capacitance for different combinations of network elements. R =R + R + … … … … . +R R R R R R R = + + … … … … . + R R L L L L L =L + L + … … … … . +L L L = + + … … … … . + L L C C C C = + + … … … … . + C C = C + C + … … … … . +C C C C Fig1.1 Series and parallel connection of circuit elements Page : 3 Network Theory Network Methodology 1.3. Voltage / Current relation in series / parallel connection of resistor Figures below summarizes voltage/current relations in series and parallel connection of resistors. i R i R i R > > > + − ≡ + − + - + V − Fig1.2 Series connection of resistor For series connection of resistors, i = i = . i = i V = Σ v , ∴ v × ∀ i = 1 , ……… n ∑ i R + V − i R i R i ≡ + V − + V − i R + V − Fig 1.3 Parallel combination of resistors For parallel connection of resistors, i = Σ i , i = i × ∀ i = 1 , ……… n Σ V = V = … … … … … … = V = V 1.4. Kirchoff’s Current Law ( KCL) KCL, states that the "total current or charge entering a junction or node is exactly equal to the charge leaving the node as it has no other place to go except to leave, as no charge is lost within the node". In other words the algebraic sum of ALL the currents entering and leaving a node must be equal to zero, I(exiting) + I(entering) = 0. This idea by Kirchoff is known as the Conservation of Charge. Page : 4 Network Theory Network Methodology Node Currents Entering the Node = Currents Leaving the Node + + = + = Fig. 1.4 Kirchoff Current Law Here, the three currents entering the node, I1, I2, I3 are all positive in value and the two currents leaving the node, I4 and I5 are negative in value. Then this means we can also rewrite the equation as; I1 + I2 + I3 - I4 - I5 = 0 The term Node in an electrical circuit generally refers to a connection or junction of two or more current carrying paths or elements such as cables and components. Also for current to flow either in or out of a node a closed circuit path must exist. We can use Kirchoff's current law when analysing parallel circuits. 1.5. Kirchoff’s Voltage Law (KVL) KVL, states that "in any closed loop network, the total voltage around the loop is equal to the sum of all the voltage drops within the same loop" which is also equal to zero. In other words the algebraic sum of all voltages within the loop must be equal to zero. This idea by Kirchoff is known as the Conservation of Energy. A B The sum of the voltage drops around the loop equal zero D C Fig. 1.5 Kirchoff Voltage Law Page : 5 Network Theory Network Methodology V + V + V + V = 0 Starting at any point in the loop continue in the same direction noting the direction of all the voltage drops, either positive or negative, and returning back to the same starting point. It is important to maintain the same direction either clockwise or anti-clockwise or the final voltage sum will not be equal to zero. We can use Kirchoff's voltage law when analysing series circuits. When analysing either DC circuits or AC circuits using Kirchoff's Circuit Laws a number of definitions and terminologies are used to describe the parts of the circuit being analysed such as: node, paths, branches, loops and meshes. These terms are used frequently in circuit analysis so it is important to understand them. Circuit - a circuit is a closed loop conducting path in which an electrical current flows. Path - a line of connecting elements or sources with no elements or sources included more than once. Node - a node is a junction, connection or terminal within a circuit were two or more circuit elements are connected or joined together giving a connection point between two or more branches. A node is indicated by a dot. Branch - a branch is a single or group of components such as resistors or a source which are connected between two nodes. Loop - a loop is a simple closed path in a circuit in which no circuit element or node is encountered more than once. Mesh - a mesh is a single open loop that does not have a closed path. No components are inside a mesh. Components are connected in series if they carry the same current. Components are connected in parallel if the same voltage is across them. Fig. 1.6 Network Methodology Representation Page : 6 Network Theory Network Methodology Example No.1 Find the current flowing in the 40Ω Resistor, R3 Fig. 1.7 The circuit has 3 branches, 2 nodes (A and B) and 2 independent loops. Using Kirchoff's Current Law, KCL the equations are given as; At node A : I1 + I2 = I3 At node B : I3 = I1 + I2 Using Kirchoff's Voltage Law, KVL the equations are given as; Loop 1 is given as : 10 = R1 x I1 + R3 x I3 = 10I1 + 40I3 Loop 2 is given as : 20 = R2 x I2 + R3 x I3 = 20I2 + 40I3 Loop 3 is given as : 10 - 20 = 10I1 - 20I2 As I3 is the sum of I1 + I2 we can rewrite the equations as; Eq. No 1 : 10 = 10I1 + 40(I1 + I2) = 50I1 + 40I2 Eq. No 2 : 20 = 20I1 + 40(I1 + I2) = 40I1 + 60I2 We now have two "Simultaneous Equations" that can be reduced to give us the value of both I1 and I2 Substitution of I1 in terms of I2 gives us the value of I1 as -0.143 Amps Substitution of I2 in terms of I1 gives us the value of I2 as +0.429 Amps As : I3 = I1 + I2 The current flowing in resistor R3 is given as : -0.143 + 0.429 = 0.286 Amps and the voltage across the resistor R3 is given as : 0.286 x 40 = 11.44 volts Page : 7 Network Theory Network Methodology The negative sign for I1 means that the direction of current flow initially chosen was wrong, but never the less still valid. In fact, the 20v battery is charging the 10v battery. 1.6. Circuit Analysis All network circuits can be solved using Kirchoff's Circuit Laws. While Kirchoff´s Laws give us the basic method for analysing any complex electrical circuit, there are different ways of improving upon this method by using Mesh Current Analysis or Nodal Voltage Analysis that results in a lessening of the math's involved and when large networks are involved this reduction in maths can be a big advantage. For example, consider the circuit from the previous example. 10 Ω 20 Ω Type equation here Type equation here 10v 20v Type equation here 40 Ω Type equation here Type equation here ( + ) Fig. 1.8 One simple method of reducing the amount of math's involved is to analyse the circuit using Kirchoff's Current Law equations to determine the currents, I1 and I2 flowing in the two resistors. Then there is no need to calculate the current I3 as its just the sum of I1 and I2. So Kirchoff's second voltage law simply becomes: Equation No 1 : 10 = 50I1 + 40I2 Equation No 2 : 20 = 40I1 + 60I2 therefore, one line of math's calculation have been saved. 1.6.1 Mesh Current Analysis A more easier method of solving the above circuit is by using Mesh Current Analysis or Loop Analysis which is also sometimes called Maxwell´s Circulating Currents method. Instead of labelling the branch currents we need to label each "closed loop" with a circulating current. As a general rule of thumb, only label inside loops in a clockwise direction with circulating currents as the aim is to cover all the elements of the circuit at least once.
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