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Small  Magnetic Loop  Antenna Design Small  Magnetic Loop  Antenna Design

Small Magnetic Loop Antenna Design - PowerPoint Presentation

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Uploaded On 2018-09-22

Small Magnetic Loop Antenna Design - PPT Presentation

Project Design Goals 1 To design and construct a small size multi band transmitting loop antenna useful for QRP and portable operation 2 To compare the performance of the loop ID: 675653

loop mhz design antenna mhz loop antenna design calculate inches vswr approximately capacitor tuning resistance khz bands diameter spreadsheet unit inductive frequency

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Slide1

Small Magnetic Loop Antenna Design

Project Design

Goals

:

1. To design and construct

a small size, multi- band transmitting

loop

antenna useful for QRP and portable operation.

2. To compare the performance of the loop

antenna

to

a known antenna type to verify performance

3. Design will cover the 40 through 15 Meter Bands inclusively

4.

To develop a computer spreadsheet to

facilitate

the

design procedure Slide2

First Generation 30 inch LoopSlide3

First Generation Design

30 inch loop using Gamma MatchSlide4

Original design used a 30 inch loop which did not tune below 14 MHz, and had efficiency issues because of the 30 inch diameter and conductor diameter (0.65 inches)The gamma match produced a current imbalance in the loop (“antenna effect”), which distorted the radiation pattern

First Generation ShortcomingsSlide5

Remote tuning

At least 30 w

power handling

capability

Portable for Field use

Cost of materials not to exceed $100.00

VSWR

less than 1.5 to 1 on all covered bands at resonance

Specific

Design

Goals Slide6

1

inch copper tubing

was investigated at first, but was dismissed because of cost and weight

.

D

esign analysis

indicated that a 42 inch diameter loop would provide a good compromise between array efficiency and frequency coverage. (ARRL Antenna Book, Antennas, by John Kraus)) A plastic gymnasium hoop

had approximately the right diameter, is low cost and light in weight

Could copper tape be used as the radiating conductor? Skin depth will have to be considered as one of the design tasks.

Selection

of materialsSlide7

6. For remote tuning, a low cost 12 volt hobby motor was selected at 0.7 RPM.

Motor

rotates in both directions

7.

The loop will use a single

coax lead-in to the

antenna

, therefore a suitable power insertion system will be designed to feed the DC control voltage up the center conductor, along with the RF signal. A control

box

with reversing polarity control voltage will be part of the design. 8. Determine the type and range of the tuning capacitor to resonate the loop

Selection of materials (continued)Slide8

1. Small loop:

A completely encircled antenna structure whose total

perimeter is below self-resonance

2. Directivity (Gain):

The ratio of loop Field Strength (in the favored direction) compared to the Field Strength of an Isotropic Radiator (or dipole)

3. Loop Efficiency (Decimal or Percent):

The ratio of Loop Radiation Resistance divided by the Sum of Radiation Resistance plus Total Loss

Resistance (Decimal). For percent, multiply decimal

value

by 100.

4. Skin Depth (Skin Effect): The distance from the top of a conducting medium where the current density decreases to 1/є of its surface value (37%) Skin Depth is denoted as δ; 86% of the total current density is contained within 2δ.

Definitions

:Slide9

Skin Depth Equation for pure copper conductor:

δ

0.002574

√ F

Where:

δ

is the skin depth in inches, and F is the Frequency in MHz

At

7 MHz, δ ≈ 0.973 x 10-3 inches 2 x

δ

=

1.95

x 10-3 inches and, At 21 MHz, δ ≈ 0.515 x 10-3 inches 2 x δ = 1.03 x 10-3 inches Calculation of Skin Depth:Slide10

Worst

case is

7 MHz,

requiring the greatest RF

current

penetration

.

Since 1 mil = 10

-3 inches, at 7 MHz, a minimum conductor thickness of 1.95 mils is required for at

least

2δ depth of current density penetration.

3M Copper

Adhesive Tape

has a conductor thickness of 2 mils, which satisfies the requirement, and was chosen for the radiating conductor. Slide11

Loop Design Procedure for Circular Loop:

1.

Choose

loop diameter,

D

, and radiator diameter,

d

, both in inches. D must be

less than

3300 where f

is the highest frequency of the loop

П f in MHZ. At 21 MHz, D must be less than 50 inches. 42 inches was chosen for this design, with radiator diameter of 1.5 inches

2. Calculate

the Loop Inductance, L

:

L

(

μ

H) = 0.005 D

x

{ [ 7.353

x

( LOG ( 8

x

D / d )] – 6.386 }

Slide12

3. Calculate the Loop Inductive Reactance, X

L,

at the highest and lowest antenna frequencies

:

X

L

= 2 x П x F x L

where:X

L

is Inductive Reactance in ohms

F is the Frequency in MHZ (highest / lowest), and L is the Loop Inductance in μH calculated in Step 2

4. Calculate the distributed loop Self Capacitance, C

S

:

C

S (pf) ≈ 0.2103 x D, with D again in inches 5. Calculate the required Capacitances to Resonate the Loop, C min and C max: C min = 106 / ( 2 x П x Fmax x XLH ) - CS, and C max = 106 / ( 2 x П x Fmin x XLL ) - CS, where: C min and C max are in pico-farads, Fmin / Fmax in MHZ XLH is the inductive reactance at the highest frequency XLL is the inductive reactance at the lowest frequency

Slide13

6. Estimate Tuning capacitor

Qc,

or use published

/ measured capacitor Qc

data. For estimate,

use

2000

to

800 for standard variable capacitor, (fully meshed to unmeshed);

and

3500 to 1000 for split rotor Butterfly

type, (fully meshed to unmeshed

). Refer to spreadsheet

Steps 7 through 17 should be performed at

the highest and lowest antenna frequencies. For these steps, XL is the inductive reactance at the associated frequency.

7

. Calculate capacitor equivalent loss resistance, R

C,

from Q

C

:

RC = XL / QC8. Calculate Loop Radiator Loss Resistance, RL: RL = ( П x D x 0.000083 x √ F ) / d, where D, d, and F are as previously defined9. Total Loss Resistance, RT, is sum of RC + RL RT = RC + RL 10. Calculate Loop Radiation Resistance, RR: RR = 9.926 x 10 -13 x F4

x

D

4

again

, where, F is in MHZ, and D as previously

definedSlide14

1

1

. Calculate antenna efficiency,

ζ

, in percent: *

ζ = {RR / (RT + RR )} x 100,

ζ

D =

ζ

/ 100, which is efficiency expressed as a decimal 12. Calculate the total Loop Antenna Q: * Q = XL / (2x( (RR + RT)) where:

XL is the Loop Inductive Reactance, and RT is the total

Loop

Loss Resistance

,

RR is radiation resistance all as previously

calculated

13. Calculate the Peak Voltage across the tuning Capacitor, VC: * VC = √ (P x XL x Q) where: P is the Peak Envelope Power driving the Loop, XL calculated from Step 3 * 14. Calculate the minimum plate spacing (inches) for the capacitor, SMin: SMin = 1.5 x VC / 50000 (Includes 1.5 to 1 safety factor at 50000 volts / in) * Choose a capacitor offering Cmin and Cmax values (Step 4), with this minimum plate spacing 15. Calculate the RMS Resonant Circulating Current in the Loop, IL: * IL ≈ 0.7071 * VC / XL, provided that XL >> RT, which is the usual case

16: Calculate Loop Bandwidth, BW

: *

BW = F / Q, where F and BW are both in MHZ. * Steps 11 through 16 are within ≈ +/- 20% if Antenna VSWR is better than 1.5 at resonance. Slide15

G dB

≈ 10

x LOG

(

ζ

D

) + 1.81

where:

G dB is the estimated free-space gain in dB

, referenced

to

an

isotropic radiator, and ζ D is the decimal value of the antenna efficiency calculated in STEP 11. 17

. Antenna Gain Estimate:Slide16

Spreadsheet permits Fast Design on Personal Computer by automating

the design steps

.

Calculates all loop parameters

except

the design of the matching / coupling network, which is determined experimentally.

Spreadsheet values are not displayed if loop size exceeds small loop criteria

Computer Aided Design by Spreadsheet:Slide17

From the Spreadsheet, the following values of Rp (Equivalent parallel resistance), are noted for a 42 inch diameter loop:

7 MHz R

P

=

62.88 K

ohms

18 MHz RP = 50.34 K ohms

21 MHz

R

P = 39.73 K ohms These values are calculated from network theory using the series to parallel transform theorem. Rp = Rs + Xs 2 / Rs Xp = Rp Rs / Xs where: Rs = Rc + Ra + Rr Xs = Loop Inductive Reactance , XL, calculated in Step 3

Can

a single matching circuit be used on all bands?

Matching Network Design:Slide18

Loop Series to Parallel

Transformation (Antenna side of Network, using Transformer Coupling)

LA

CA

LA

CASlide19

VSWR on 7 MHz:

VSWR

7

MHz

= R

P

7

MHz / R

P

18 MHz

=

62.88 / 50.34 = 1.25 VSWR on 21 MHz: VSWR 21 MHz = RP

18 MHz

/

R

p 21

MHz = 50.34 / 39.73 = 1.27 From above data, a single coupling loop match of proper spacing would meet the design goal of VSWR less than 1.5 on all bands Design a matching circuit to be close to a perfect match at ≈ 18 MHz, calculate the expected VSWR on the band edges.Slide20

Realization of

Transformer

Match

Secondary coupling loop approx 1/5 diameter of main loop, distance determined experimentallySlide21

Transformer match detailSlide22

Loop after construction and Initial Tests:Slide23

Photo

of

Tuning Unit:Slide24
Slide25

Tuning Unit Schematic DiagramSlide26

Control Box Photograph:Slide27
Slide28

VSWR (measured using MFJ-469 Analyzer

):

7 MHz

1.2

10 MHz 1.3

14 MHz

1.3 18 MHz

1.1

21 MHz

1.3 7 – 21 MHz Met the design goal of VSWR < 1.5 Tuning Time: Approximately 35 seconds 7 MHz to 21 MHz

Qualitative Gain (switching back-and-forth compared

to ground mounted vertical (one

hop

propagation )

7 MHz

vertical better by approximately 1 S Unit 10 MHz vertical better by approximately ½ S Unit 14 MHz no discernible difference 18 MHz approximately ½ S Unit better on loop 21 MHz approximately ½ S Unit better on loopAntenna was mounted in vertical orientationPower Capability: Tuning Capacitor warm to the touch at 30 watts when keyed for 30 seconds on 7, 10, and 14 MHz bands. Antenna slightly warm on 7 MHz band. No evidence of arcing on any band at 30 watts. Very little capacitor temperature rise noted on 18 and 21 MHz bands. Antenna, itself did not show any rise in temperature on bands above 7 MHz. Measured Performance:Slide29

2.6 to 1 VSWR Bandwidth:

Measured Spreadsheet

7 MHz

approximately

12 KHz 11.2 KHz

10 MHz approximately 20 KHz 19.9 KHz

14 MHz approximately

46 KHz 43.2 KHz

18 MHz approximately 96 KHz 92.5 KHz

21 MHz

approximately

170 KHz 159.6 KHz Measurements are in close agreement with the Spreadsheet.Measured Performance (Continued):Slide30

Item Qty Unit Price Ext

Control Box Plastic enclosure 1 3.50 3.50

Antenna Tuning enclosure 1 6.50 6.50

Hobby motor

0.7

rpm

1

5

.50

5.50Variable

Capacitor (20 -360 pf)

1 20.50 20.50SO-239 connectors 3 3.00 9.00.875 in OD Type 43 Ferrite 3 2.00 6.00Tantalum Capacitors 2 2.00 4.00Disc Capacitors 10 .25 2.5010 volt regulator (LM-7810) 1 1.50 1.501N4007 Diode 2 .25 .5042 in Snap Together Hoop (Amazon) 1

9

.00

9

.00

Dip mica capacitors 3 .50 1.50

Vector Board 1

.50 .50DPDT Momentary Switch 1 2.50 2.502 pin Power connector with mate 3 2.50 2.00Miscellaneous wire and hardware A/R 2.00 (est) 2.00Copper Tape (average 1 roll) A/R 12.00 (est) 12.00 Total $89.50 Priced Bill of Materials:Slide31

1. Design

goal was achieved, to construct a low cost,

small size

loop antenna.

2. VSWR was less than 1.5 on all bands using a single

Coupling Loop

Match section

3.

Qualitative Gain performance was within 1 S Unit of ground mounted vertical mono-pole on 7 and 10 MHz, equal or better on higher bands .

4. Power

handling up to 30 watts PEP.5. Priced Bill of

materials less

than the design goal budget of $100.00

6. Could be an attractive antenna for portable use, or by an amateur who does not have the space for a full sized outdoor antenna

7. Spreadsheet is available via email (Excel) Any Questions? Thank you and See you all on the air 73 de WY2U

Mike Kozma dmkozma@optonline.net

Summary

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