CM Corner Reflector by K6STI
CE Converted with 4nec2 on 22-apr-02
SY S = -10
SY A = 16
SY B = 11
SY D = .375
GW	1	11	B	-5.85	0	B	5.85	0	D
GW	2	10	0	-A	0	0	A	0	D
GW	3	10	2	-A	2	2	A	2	D
GW	4	10	4	-A	4	4	A	4	D
GW	5	10	6	-A	6	6	A	6	D
GW	6	10	8	-A	8	8	A	8	D
GW	7	10	10	-A	10	10	A	10	D
GW	8	10	12	-A	12	12	A	12	D
GW	9	10	14	-A	14	14	A	14	D
GW	10	10	16	-A	16	16	A	16	D
GW	11	10	18	-A	18	18	A	18	D
GW	12	10	20	-A	20	20	A	20	D
GW	13	10	22	-A	22	22	A	22	D
GW	14	10	2	-A	-2	2	A	-2	D
GW	15	10	4	-A	-4	4	A	-4	D
GW	16	10	6	-A	-6	6	A	-6	D
GW	17	10	8	-A	-8	8	A	-8	D
GW	18	10	10	-A	-10	10	A	-10	D
GW	19	10	12	-A	-12	12	A	-12	D
GW	20	10	14	-A	-14	14	A	-14	D
GW	21	10	16	-A	-16	16	A	-16	D
GW	22	10	18	-A	-18	18	A	-18	D
GW	23	10	20	-A	-20	20	A	-20	D
GW	24	10	22	-A	-22	22	A	-22	D
GM	0	0	0	0	0	-B	0	0	1
'GX	1	010	' Add when needed.
GS	0	0	in
GE	0
EX	0	1	5	00	1.0	0.0
'
GN	-1
FR	0	1	0	0	 432
EN
'compared with a yagi, gain per conductor-wavelength for a corner reflector is
'very low.  However, when a bowtie dipole is used, good gain over an octave
'bandwidth can be obtained.  This is not possible with a Yagi.  For more
'information, see "Antennas" by John Kraus, 2nd ed., pp 549-560.