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Pictorial Method You can use a protractor and a ruler to find phase angles for RC circuits, just as you did with RL circuits in the previous chapter, as long as the angles aren t too close to 0 or 90 . First, draw a line somewhat longer than 10 cm, going from left to right on the paper. Then, use the protractor to construct a line going somewhat more than 10 cm vertically downward, starting at the left end of the horizontal line. The horizontal line is the R axis of an RC plane. The line going down is the X C axis. If you know the actual values of X C and R, divide or multiply them by a constant, chosen to make both values fall between 100 and 100. For example, if X C = 3800 and R = 7400 , divide them both by 100, getting 38 and 74. Plot these points on the lines. The X C point goes 38 mm down from the intersection point between your two axes. The R point goes 74 mm to the right of the intersection point. Next, draw a line connecting the two points, as shown in Fig. 14-11. This line will be at a slant and will form a triangle along with the two axes. This is a right triangle, with the right angle at the origin of the RC plane. Measure the angle between the slanted line and the R axis. Use the protractor for this. Extend the lines, if necessary, using the ruler, to get a good reading

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ATM is a cell-based technology, which simply means that the fundamental unit of transport a frame of data, if you will is of a fixed size, which enables switch designers to build faster, simpler devices, because they can always count on their switched payload being the same size at all times That cell comprises a 5-octet header and a 48-octet payload field, as shown in Figure 6-5 The payload contains user data and the header contains information that the network requires to both transport the payload correctly and ensure proper quality of service levels for the payload ATM accomplishes this task well, but at a cost The 5-octet header comprises nearly 10 percent of the cell, a rather significant price to pay,.

This will be important later, when you need to work with inductive and capacitive reactances together in the same circuits..

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on the protractor. This angle will be between 0 and 90 . Multiply this reading by 1 to get the RC phase angle. That is, if the protractor shows 27 , the RC phase angle is 27 . The actual vector is found by constructing a rectangle using the origin and your two points, making new perpendicular lines to complete the figure. The vector is the diagonal of this rectangle, running out from the origin (Fig. 14-12). The phase angle is the angle between the R axis and this vector, multiplied by 1. It will have the same measure as the angle of the slanted line you constructed in Fig. 14-11.

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In many ways capacitive reactance behaves like a mirror image of inductive reactance. But in another sense, XC is an extension of XL into negative values below zero. If the frequency of an ac source is given in hertz as f and the capacitance of a capacitor in farads as C, then the capacitive reactance is XC 1/(6.28fC)

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method of finding phase angle in a circuit containing resistance and capacitive reactance. This method shows the actual impedance vector.

This same formula applies if the frequency, f, is in megahertz and the capacitance, C, is in microfarads ( F). Just remember that if the frequency is in millions, the capacitance must be in millionths. Capacitive reactance varies inversely with the frequency. This means that the function XC vs f appears as a curve when graphed, and this curve blows up as the frequency nears zero.

6

Trigonometric Method Using trigonometry, you can determine the RC phase angle more precisely than the pictorial method allows. Given the values of X C and R, the RC phase angle is the arctangent of their ratio. Phase angle in RC circuits is symbolized by the lowercase Greek letter , just as it is in RL circuits. Here are the formulas:

250 Capacitive reactance Capacitive reactance also varies inversely with the actual value of capacitance, given a fixed frequency. Therefore, the function of XC vs C also appears as a curve that blows up as the capacitance approaches zero. The negative of Xc is inversely proportional to frequency, and also to capacitance. Relative graphs of these functions are shown in Fig. 14-4.

particularly when other technologies such as IP and SONET add their own significant percentages of overhead to the overall payload. This reality is part of the problem. ATM s original claims to fame, and the reasons it rocketed to the top of the technology hit parade, were its capability to switch cells at tremendous speeds through the fabric of the WAN and the ease with which the technology could be scaled to fit any network situation. Today, however, given the availability of high-speed IP routers that routinely route packets at terabit rates, ATM s advantages have begun to pale to a certain degree.

= tan 1 (X C /R ) or = arctan (XC /R )

Problem 14-1

A capacitor has a value of 0.00100 F at a frequency of 1.00 MHz. What is the capacitive reactance Use the formula and plug in the numbers. You can do this directly, since the data is specified in microfarads (millionths) and in megahertz (millions): XC 1/(6.28 1.0 0.00100) 1/(0.00628) 159

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