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Balanced and Unbalanced Loads and Lines A balanced load is one whose terminals can be reversed without significantly affecting circuit behavior A plain resistor is a good example The two-wire antenna input in a television receiver is another example of a balanced load A balanced transmission line is usually a two-wire line, such as oldfashioned TV ribbon, also called twinlead An unbalanced load is a load that must be connected a certain way Switching its leads will result in improper circuit operation In this sense, an unbalanced load is a little like a polarized component such as a battery or capacitor Many wireless antennas are of this type Usually, unbalanced sources and loads have one side connected to ground The coaxial input of a television receiver is unbalanced; the shield (braid) of the cable is grounded An unbalanced transmission line is usually a coaxial line, such as you find in a cable television system Normally, you cannot connect an unbalanced line to a balanced load, or a balanced line to an unbalanced load, and expect good performance But a transformer can allow for mating between these two types of systems In Fig 18-10A, a balanced-to-unbalanced transformer is shown Note that the balanced side is center-tapped, and the tap is grounded In Fig 18-10B, an unbalanced-tobalanced transformer is illustrated Again, the balanced side has a grounded center tap The turns ratio of a balanced-to-unbalanced transformer (also called a balun) or an unbalancedto-balanced transformer (also known as an unbal) can be 1:1, but this need not be the case, and often it is not If the impedances of the balanced and unbalanced parts of the systems are the same, then a 1:1 turns ratio is ideal But if the impedances differ, the turns ratio should be such that the impedances are matched Shortly, we ll see how the turns ratio of a transformer can be manipulated to transform one purely resistive impedance into another Transformer Coupling Transformers are sometimes used between amplifier stages in electronic equipment where a large amplification factor is needed There are other methods of coupling from one amplifier stage to another, but transformers offer some advantages, especially in RF receivers and transmitters Part of the problem in getting a radio to work is that the amplifiers must operate in a stable manner If there is too much feedback, a series of amplifiers will oscillate, and this will severely degrade the performance of the radio Transformers that minimize the capacitance between the amplifier stages, while still transferring the desired signals, can help to prevent this oscillation.

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significant figures, is 89 The circuit contains an almost pure inductive reactance, because the phase angle is close to 90 The resistance contributes little to the behavior of this RL circuit at 10 MHz

1 + 0001931851353 sin2 ( ) 1 00066943800229 sin2 ( )

The vector [ g , g , g ] represents local perturbations in the gravity vector relative to the ellipsoidal normal vector Both gg and [ g , g , g ] are functions of position, but the argument is not shown to simplify the notation

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Problem 13-6 What is the phase angle for the preceding circuit at a frequency of 10 kHz With that information, what can we say about the behavior of the circuit at 10 kHz This requires that XL be calculated again, for the new frequency Let s use megahertz, so it goes in the formula with microhenrys A frequency of 10 kHz is the same as 0010 MHz Calculating, we get XL = 628fL = 628 0010 90 = 565 The ratio XL/R is 565/10 = 0565 Therefore, the phase angle is arctan 0565, which, rounded to two significant figures, is 29 This is not close to either 0 or 90 Thus, at 10 kHz, the resistance and the inductive reactance both play significant roles in the behavior of the circuit

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This section presents algorithms to transform between the geodetic (ie, ( , , h)e ) and rectangular (ie, (x, y, z)e ) ECEF coordinates The WGS84 ellipsoid parameters are used throughout the discussion When the geodetic coordinates are known, the coordinates in the ECEF frame is calculated as x = (RN + h) cos( ) cos( ) y = (RN + h) cos( ) sin( ) z = [RN (1 e2 ) + h] sin( ) (29) (210) (211)

Example 21 The geodetic position of a point in the vicinity of Los Angeles, CA is = 34 degrees, 0 minutes, 000174 seconds North, = 117 degrees, 20 minutes, 084965 seconds West, and h = 251702 m These coordinates convert to = 05934119541 rad and = 20478571082 rad The signs and precision are critical, see Exercise 23 Then RN = 6384823214 106 m and [x, y, z]e = [ 2430601828, 4702442703, 3546587358] m (212)

Refer to the text in this chapter if necessary A good score is 18 correct Answers are in the back of the book 1 As the number of turns in a coil that carries ac increases without limit, the current in the coil will (a) eventually become very large (b) stay the same (c) decrease, approaching zero (d) be stored in the core material 2 As the number of turns in a coil increases, the reactance at a constant frequency (a) increases (b) decreases (c) stays the same (d) is stored in the core material 3 As the frequency of an ac wave gets lower, the value of XL for a particular coil of wire (a) increases (b) decreases (c) stays the same (d) depends on the voltage 4 Suppose a coil has an inductance of 100 mH What is the reactance at a frequency of 1000 Hz (a) 0628 (b) 628 (c) 628 (d) 628

Readers unfamiliar with the degrees, minutes, seconds notation should see Exercises 23 and 24 The transformation from [x, y, z]e to geodetic coordinates is more involved, but is important in GPS applications where the ECEF rectangular coordinates are directly determined from range measurements and the

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