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and to add the two phasors using the familiar techniques of complex algebra However, this approach would be incorrect Whenever a sinusoidal signal is expressed in phasor notation, the term ej t is implicitly present, where is the actual radian frequency of the signal In our example, the two frequencies are not the same, as can be veri ed by writing the phasor currents in the form of equation 446: I1 = Re [A1 ej 0 ej 1 t ] I2 = Re [A2 ej 0 ej 2 t ] (451)

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Since phasor notation does not explicitly include the ej t factor, this can lead to serious errors if you are not careful! The two phasors of equation 450 cannot be added, but must be kept separate; thus, the only unambiguous expression for the load current in this case is equation 448 In order to complete the analysis of any circuit with multiple sinusoidal sources at different frequencies using phasors, it is

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Assuming 12.5 map units (or a probability of 0.125 of a crossover; 0.125), the probability of child III-1 is 0.4375. This child would be a nonrecombinant, so his probability of having the nail-patella syndrome and type A blood is half the probability of no crossover during meiosis, or (1 0.125)/2. We divide by two because there are two nonrecombinant types. This is the same probability for all children except III-5, whose probability of occurrence is 0.125/2 0.0625, since he is a recombinant. Thus, the numerator of the previous equation is (0.4375)7(0.0625). If the two loci are not linked, then any genotype has a probability of 1/4, or 0.25. Thus, the sequence of the eight children has the probability of

(455)

Recombination Frequency ( )

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Equation 455 corresponds to Ohm s law in phasor form, and the result should be intuitively appealing: Ohm s law applies to a resistor independent of the particular form of the voltages and currents (whether AC or DC, for instance) The ratio of phasor voltage to phasor current has a very simple form in the case of the resistor In general, however, the impedance of an element is a complex function of frequency, as it must be, since it is the ratio of two phasor quantities, which are frequency-dependent This property will become apparent when the impedances of the inductor and capacitor are de ned The Inductor Recall the de ning relationships for the ideal inductor (equations 49 and 412), repeated here for convenience: vL (t) = L 1 iL (t) = L diL (t) dt vL (t )

Fig 239: (a) Synthesis of cubic boron nitride [32] using magnesium as a catalyst (b) An insert consisting of cubic

(456)

0.05 0.10 0.125 0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50

Let vL (t) = vS (t) and iL (t) = i(t) in the circuit of Figure 433 Then the following expression may be derived for the inductor current: iL (t) = i(t) = iL (t) = = 1 L 1 L vS (t ) dt (457)

Note how a dependence on the radian frequency of the source is clearly present in the expression for the inductor current Further, the inductor current is shifted in phase (by 90 ) with respect to the voltage This fact can be seen by writing the inductor voltage and current in time-domain form: vS (t) = vL (t) = A cos t i(t) = iL (t) = A cos t L 2 (458)

0.951 1.088 1.099 1.090 1.031 0.932 0.801 0.643 0.457 0.244 0.000

It is evident that the current is not just a scaled version of the source voltage, as it was for the resistor Its magnitude depends on the frequency, , and it is shifted (delayed) in phase by /2 radians, or 90 Using phasor notation, equation 458 becomes VS (j ) = A 0 I(j ) = A /2 L (459)

boron nitride and tungsten carbide compact Only four cutting edges are available (c) A micrograph of cubic boron nitride on a WC+Co substrate (Etchant: Murakami)[3]

HPRT TK in the presence of Sendai virus or polyethylene glycol. Fusion takes place in some of the cells, and the mixture is grown in a medium containing hypoxanthine, aminopterin, and thymidine (called HAT medium). In the presence of aminopterin, unfused mouse cells (TK ) and unfused human cells (HPRT ) die. Hybrid cells, however, survive because they are

Thus, the impedance of the inductor is de ned as follows: VS (j ) = L /2 = j L I(j )

ZL (j ) =

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