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6.5 Power Flux Density The power flux density of a radio wave is a quantity used in calculating the performance of satellite communications links. The concept can be understood by imagining the transmitting antenna to be at the center of a sphere. The power from the antenna radiates outward, normal to the surface of the sphere, and the power flux density is the power flow per unit surface area. Power flux density is a vector quantity, and its magnitude is given by E2 ZW (6.3)

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Here, E is the rms value of the field given by Eq. (6.1). The units for are watts per square meter with E in volts per meter and ZW in ohms. Because the E field is inversely proportional to distance (in this case the radius of the sphere), the power density is inversely proportional to the square of the distance. 6.6 The Isotropic Radiator and Antenna Gain The word isotropic means, rather loosely, equally in all directions. Thus an isotropic radiator is one which radiates equally in all directions. No real antenna can radiate equally in all directions, and the isotropic radiator is therefore hypothetical. It does, however, provide a very useful theoretical standard against which real antennas can be compared. Being hypothetical, it can be made 100 percent efficient, meaning that it radiates all the power fed into it. Thus, referring back to Fig. 6.1a, Prad PS. By imagining the isotropic radiator to be at the center of a sphere of radius r, the power flux density, which is the power flow through unit area, is PS

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How should the lengths and angles be calculated Refer to your math textbooks, all the formulas are there, they are similar to the formulas given in Fig 106 1014 DRAWING ANY SHAPE As you may have noticed from the previous sections, all that is needed to draw any shape is the correct set of instructions to make the robot turn and move Combining this with the ability to put the pen up and down you can make the robot draw any shape One way to achieve this easily is to use the Data command to create an array of data pairs where each pair represents a command for the robot The rst element of the pair.

4 r2

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01 //---Draw Any Shape 02 MainProgram: 03 //----change these to make the shape have 04 //----different orientation and position 05 R_Init_X = 400 06 R_Init_Y = 300 07 R_Init_Heading = 90 08 rLocate R_Init_X,R_Init_Y,R_Init_Heading 09 rInvisible Magenta 10 LineWidth 4 11 Data SomeShape; "p",Down, "f",165, "t",-120, "f",58 12 Data SomeShape; "t",-60, "f",50, "t",-30, "f",100 13 Data SomeShape; "p",Up, "f",40 14 for I = 1 to MaxDim(SomeShape,1)/2 15 J = (I-1)*2 16 if SomeShape[J] = "f" then rForward SomeShape[J+1] 17 if SomeShape[J] = "t" then rTurn SomeShape[J+1] 18 if SomeShape[J] = "p" then rPen SomeShape[J+1] 19 next 20 End

37.19 What identity is implied by the result of Problem 37.18(i)

(6.4)

Now the flux density from a real antenna will vary with direction, but with most antennas a well-defined maximum occurs. The gain of the antenna is the ratio of this maximum to that for the isotropic radiator at the same radius r: G

speci es an action to be taken. The second element provides a parameter associated with the action. Let s look at some examples. We can use the pair f , 20 to tell the robot to move forward 20 pixels. The pair t , 40 means turn 40 and p , Up tells the robot to put the pen Up. Based on these commands, what shape would this set of data draw

37.20 Find the following antiderivatives: dx (a) (b) 4 + x2 dx (f ) (e) (x 3) x 2 6x + 8 dx (i) (j) x 9x 2 16 (m) (q) dx 6x x 2 x dx 4 x4 (n) (r)

(6.5)

Data SomeShape; p ,Down, f ,165, t ,-120, f ,58 Data SomeShape; t ,-60, f ,50, t ,-30, f ,100 Data SomeShape; p ,Up, f ,40

A very closely related gain figure is the directivity. This differs from the power gain only in that in determining the isotropic flux density, the

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