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Vector Representation of Impedance Any impedance R + jX can be represented by a complex number of the form a + jb Just let R = a and X = b Now try to envision how the impedance vector changes as either R or X, or both, are varied If X remains constant, an increase in R causes the vector to get longer If R remains constant and XL gets larger, the vector grows longer If R stays the same but XC gets larger negatively, the vector grows longer Think of the point R + jX moving around in the RX plane, and imagine where the corresponding points on the axes lie These points can be found by drawing dashed lines from the point R + jX to the R and X axes, so that the dashed lines intersect the axes at right angles Some examples are shown in Fig 15-6 Now think of the points for R and X moving toward the right and left, or up and down, on their axes Imagine what happens to the point R + jX in various scenarios This is how impedance changes as the resistance and reactance in a circuit are varied Resistance is one-dimensional Reactance is also one-dimensional But impedance is twodimensional To fully define impedance, you must render it on a two-dimensional coordinate system such as the RX plane The resistance and the reactance can change independently of one another

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Next, we get the matrix into echelon form, which looks like this:

protein (grams) 085 162 1278 839 000

# 0 0 # # 0 # # # # # #

fat (grams) 033 020 158 139 10000

.

where a pound sign (#) can represent any real number Then we go for the diagonal form:

@ 0 0 0 @ 0 0 0 @ # # #

carbohydrate (grams) 464 237 7469 8070 000

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Absolute-Value Impedance You ll occasionally read or hear that the impedance of some device or component is a certain number of ohms For example, in audio electronics, there are 8- speakers and 600- amplifier inputs How, you ask, can manufacturers quote a single number for a quantity that is two-dimensional and needs two numbers to be completely expressed That s a good question, and there are two answers First, figures like this refer to devices that have purely resistive impedances, also known as nonreactive impedances Thus, the 8- speaker really has a complex impedance of 8 + j0, and the 600- input circuit is designed to operate with a complex impedance at, or near, 600 + j0 Second, you can talk about the length of the impedance vector (that is, the absolute value of the complex impedance), calling this a certain number of ohms If you talk about impedance this way, however, you are being ambiguous There can exist an infinite number of different vectors of any given length in the RX plane Sometimes, the uppercase italic letter Z is used in place of the word impedance in general discussions This is what engineers mean when they say things like Z = 50 or Z = 300 nonreactive In this context, if no specific impedance is given, Z = 8 can theoretically refer to 8 + j0, 0 + j8, 0 j8, or any other complex impedance point on a half circle consisting of all points 8 units from 0 + j0 This is shown in Fig 15-7 Problem 15-4 Name seven different complex impedances that can theoretically be meant by the expression Z = 10 It s easy name three: 0 + j10, 10 + j0, and 0 j10 These represent pure inductance, pure resistance, and pure capacitance, respectively A right triangle can exist having sides in a ratio of 6:8:10 units This is true because 62 + 82 = 2 10 (Check it and see!) Therefore, you can have 6 + j8, 6 j8, 8 + j6, and 8 j6, all complex impedances whose absolute value is 10.

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where a pound sign can represent any real number, and an at sign (@) can represent any nonzero real number Our final goal is the unit diagonal form:

sodium (milligrams) 900 800 700 50820 000

Once we ve put a matrix into the unit diagonal form, we may find that one or more of the solutions x, y, or z is a fraction that can be reduced We ought to reduce all solutions to their lowest forms in the interest of elegance

Impedance Transfer Ratio In RF and AF systems, transformers are employed to match impedances Thus, you will sometimes hear or read about an impedance step-up transformer or an impedance step-down transformer The impedance transfer ratio of a transformer varies according to the square of the turns ratio, and also according to the square of the voltage-transfer ratio If the primary (source) and secondary (load) impedances are purely resistive and are denoted Zpri and Zsec, then the following relations hold:

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