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and label the open-circuit voltage, vOC Next, we observe that, since vb is equal to the reference voltage, (ie, zero), the node voltage va will be equal, numerically, to the open-circuit voltage If we de ne the other node voltage to be v, nodal analysis will be the natural technique for arriving at the solution Figure 350 depicts the original circuit ready for nodal analysis Applying KCL at the two nodes, we obtain the following two equations: 12 v v v va =0 1 10 10 va v va =0 10 20 In matrix form we can write: 12 01 01 015 v va = 12 0

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the crater recedes when a coating is present, leading to the development of a wider stagnant zone [16]

Comments: Note that the determination of the Th venin voltage is nothing more than e the careful application of the basic circuit analysis methods presented in earlier sections The only difference is that we rst need to properly identify and de ne the open-circuit load voltage You will nd the solution to the same example computed by MathCad in the electronic les that accompany this book

Alix (Alexandra) (1872 1918)

R2 = 12

Tsar Nicholas II of Russia (1868 1918)

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Assumptions: Assume reference node is at the bottom of the circuit Analysis: We rst compute the Th venin equivalent resistance According to the method e proposed earlier, we zero the two sources by shorting the voltage source and opening the current source The resulting circuit is shown in Figure 352 We can clearly see that RT = R1 R2 = 4 12 = 3 Following the Th venin voltage methodology box, we rst remove the load and label e the open-circuit voltage, vOC The circuit is shown in Figure 353 Next, we observe that, since vb is equal to the reference voltage (ie, zero) the node voltage va will be equal, numerically, to the open-circuit voltage In this circuit, a single nodal equation is required to arrive at the solution:

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In these tools, crater wear begins at a distance from the coating edge [Figure 210 (b)], and the wear moves towards the cutting edge with further machining [17] A small width of the cutting edge with the crater front is maintained even after a long period of machining The retention of the sharp front lip at the cutting edge provides a longer tool life But as the crater depth increases, the front lip becomes weak, which may lead to chipping of the cutting edge due to the high brittleness of the coating

Irene (1866 1953)

va R1 I V + _ R2 + vOC vb 3 i 27 V + _ 6

Finally, we assemble the Th venin equivalent circuit, shown in Figure 354, and e reconnect the load resistor Now the load current can be easily computed to be: i= 27 vT =3A = RT + R L 3+6

Victoria (1887 1969)

Comments: It may appear that the calculation of load current by the Th venin equivalent e method leads to more complex calculations than, say, node voltage analysis (you might wish to try solving the same circuit by nodal analysis to verify this) However, there is one major advantage to equivalent circuit analysis: Should the load change (as is often the case in many practical engineering situations), the equivalent circuit calculations still hold, and only the (trivial) last step in the above example needs to be repeated Thus, knowing the Th venin equivalent of a particular circuit can be very useful whenever we e need to perform computations pertaining to any load quantity

318 With reference to Figure 346, nd the load current, iL , by mesh analysis, if vS = 10 V, R1 = R3 = 50 , R2 = 100 , RL = 150

Olga (1895 1918)

223 Coating of the First Generation of TiC (Cermets)

319 Find the Th venin equivalent circuit seen by the load resistor, RL , for the circuit e of Figure 355 320 Find the Th venin equivalent circuit for the circuit of Figure 356 e

Marie (1899 1918) Anastasia (1901 18)

05 A 60

+ 15 V 025 A _

Alexis (1904 18)

Computing the Norton Current The computation of the Norton equivalent current is very similar in concept to that of the Th venin voltage The following de nition will serve as a starting point: e

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