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A normal yield is a sign of a stable interest-rate picture for the time being. If the curve begins to become misshapen, there may be anticipation or expectation building in the market for changes in interest rates. As the threat of interest-rate changes increases or actual short-term interest rates such as the Fed rate begin to increase, there will be changes in the yield curve. Most nancial news Web sites and services produce a daily yield curve, especially on Treasury issues. As short-term rates begin to rise, the curve will become more shallow, meaning that the yield is increasing on the short-term instruments in relation to the long-term secondary market instruments. This change indicates a potential need for action in your portfolio in any interest-rate sensitive areas such as xed income securities. Let s look at an example of a changing yield curve shown in Figure 10.2. In the at yield curve we can see that short-term rates are beginning to increase, which in the case of Treasuries would be T-bills or short-term T-notes. The yield is beginning to balance between

T-68 ferrite core Inductors L2 and L4 consist of 12 turns of 22 ga AWG wire on an FT37-43 ferrite core, and finally L3 consists of 25 turns of #26 ga AWG wire on a T50-2 ferrite core For even greater selectivity (but greater insertion loss), you can consider moving the L1 tap to 1 turn from ground Fine tuning the WWV receiver is accomplished by adjusting CV1 and CV2 trimmer capacitors The front-end MOSFETs are extremely sensitive to static electricity, so be very careful in handling them Note the two ferrite beads, one is placed in series with the Drain lead of Q1, while the second ferrite bead is in series with the Drain of Q2 These ferrite beads are important, so be sure to use them The receiver front-end, at J1, should be connected to a dipole antenna cut for 10 MHz.

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Taking the partial derivative of J with respect to x and setting it equal to zero yields J = Fk y f (xk ) + Fk (x xk ) = 0. x Using the solution of this equation as the next estimate of the minimum xk+1 yields the algorithm xk+1 = xk + Fk Fk

FIGURE 5-6

TRF receivers are especially sensitive and are subject to overloading a BCB or Broadcast Band Interference, so internal lead lengths should be kept short between components and the front-end should be shielded and the receiver placed in a metal enclosure for best results The output impedance of Q2 is 2000 ohms, which nicely matches the input impedance of the Cohn crystal filter, in the crystal filter section of the receiver This filter utilizes three 10 MHz crystals Choose 10 MHz crystals that are marked for a 20 pF or 32 pF load capacitance if possible Using a 10 MHz crystal oscillator, find three that are closest to one another in frequency You may substitute 22k ohm resistors instead of the specified 2k with a slight penalty in pass band shape The crystal filter section utilizes a single dual-gate MOSFET transistor at Q3.

You specify the name of the array object and the name of the property (length) separated by a dot to access the length property. In this example, the length of the array is assigned to the variable len.

l-i. 19 Temperatures are measuredat various pointsona at 0 . 5 0 0 0 heated plate (Table P15.19). Estimate the temperature ( 0 0 0 0 0 ( a ) . r : 4 , ) ' : 3 . 2 , a n d b ) r : 4 . 3 .y : 2 ; 7 . 15.20 Use the portion of the given stearntablefor superheated HrO at 200 MPa to (a) tind the conesponding D e t e r m i n ea l t : 0 . 2 3 . i entropys for a specificvolurne u of 0.108 mi/kg with linear l5.llJ The acceleration due to gravity at an altitudey above interpolation, find the samecorresponding (b) entropy usrng the surfaceof the earth is given by quadraticinterpolation, and (c) find the volumeconespond. ir-rg an entropyof 6.6 using inverseinterpolation. to a 0 01250 624 02500 775 03250 4.85

Coil L5 is 12 turns on an FT37-43 ferrite core The output of the Cohn crystal filter is next fed to the input of the AM detector stage..

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