First of all, a monopole magnet cannot exist because the two poles are a single entity. That is made very clear in this image showing the views from each side of an electromagnet coil. The current flow is clearly in opposing directions when viewed from each side and it's obvious that the changing charge relationship between the charges as the electron flow progresses around the coil is the foundation of a magnetic field.
The relationship between the charges of a material is continuously updating at the speed of light. If a charge relationship changes in any way, a recording of the change expands outward from the source into the past at light speed. The changing charge relationship must always occur at a specific rate and in a specific direction.
(animation) 
The single pulse transmitter and the receiver are spaced far enough apart so that the static electric field is of little consequence.
There is no doubt at all that the charges in the receiver will temporarily react to changes in the transmitter in exactly the manner indicated. There is also no doubt that the entire process, including the action of the magnetic field, is occurring in the plane of dimension along which the charge relationship in the antenna is changing.
When the charge difference between the transmitter ends is at its maximum, the momentarily static electric field flux lines over the length of the conductor range between the greatest charge density of one sine to the greatest charge density of the opposite sine. A plot of equal charge density of one sine or the other can be found at any radius perpendicular to the axis of the electron movement along the transmitter length. And that's exactly where the strength of the magnetic field flux lines are found to be isotropic as well. In a sense, the two fields are identical.
When electrons are flowing along the transmitter length in the process of inverting the charge on the ends, they are in motion relative to their fixed e+ counterparts. The electric field between every charge is being indexed along from one association to the next in line. The electric flux lines in a closer relationship with the action in the transmitter are indexed along at a greater rate, or more intense rate than the more distant flux lines. That action sets up rotation in much the same way as an air jet stirs the surrounding air mass.
An analogy for magnetic attraction and repulsion can be taken from two air masses rotating in the same direction around the same point, in the same plane, while being driven from individual sources. But in this case, every molecule of each air mass is driven from its specific source drive. They will strongly resist any misalignment between the centers of rotation. Spin one air mass in the opposite direction and the two will be forced apart.
From your viewpoint of the transmitter, when the charges are in the process of inverting to -- at the top and ++ at the bottom, the rotating electric field stirred into action by the more intense drive close to the transmitter body, is cycling anticlockwise on the left hand side of the transmitter body and clockwise on the right hand side. You see a south pole on the left and a north pole on the right. The two poles of a magnet are simply views of the same rotating electric fields taken from opposite sides.
While the magnetic field is constant at any point along the transmitter, no current flow would be induced in either direction in a conductor that's moving around the transmitter axis at a constant radius about its centerline because the moving electric and magnetic fields remain isotropic throughout the motion.
The flux lines in this image were generated by two, very long parallel conductors that are connected to form a closed loop circuit. The distance ratio between the two conductors and a specific point on any field line is exactly the same for every other point around that field line.
The next image was generated for one specific field line. Each set of circles is expanded by exactly the same ratio for each step. Where they intersect is the point where the ratio of input between conductors is constant for each step. Notice that the input from each conductor reduces at a linear rate, in a single plane of dimension, as should be expected because the relationship between charged particles (matter) can only change in a single plane of dimension at any time, and that changing relationship is exactly what creates the magnetic field.
The figures shown are for the two radii in pixels for the final set of intersecting curves. Every curve set in that plot has a constant ratio between the two radii, which is 1.5 to 1. The flux line origin was set at 40 on the scale shown.
When a constant current is flowing in an electromagnet coil, electric field change is occurring throughout the coil and the recording of each change MUST BE TRANSMITTED, but no matter what shape the coil is, because the power in the transmission of every change in the coil reduces at a linear rate the combined drive in any direction from the closed loop circuit arriving at any (stationary relative to the coil) point must always equal zero. The proof of this is in every magnetic field. One only needs to shift an appropriate detector across flux lines to see this proof (with eyes open of course).
Clearly, electromagnetic radiation is manifested out of changes occurring within a charge structure, and those changes have occurred in a specific direction and at a specific rate relative to the rigid e+ charge structure.
There is no reason whatever to assume that an accelerating charge will transmit any sort of signal purely from the action of its acceleration. The most significant distortion surrounding an accelerating charge is in the direction of the acceleration, and the most significant wave emitted from this action should be a compression-rarefaction wave, not the wave formed in the direction of the "kink" wave which is formed perpendicular to the acceleration path, where the acceleration direction is of no significance at all.
The emissive power from a change to a charge structure, which can only possibly occur in a single plane of dimension, reduces by two per doubling of distance in the radial plane perpendicular to the axis of the change direction, while the apparent length of a receiver oriented in the plane of the changing charge structure also reduces by two per doubling of distance to the receiver. So the received power reduces by four per doubled distance.
This is the program which generated the field lines. Copy the program directly off the I.E (full) screen and paste it into Notepad (no wordwrapping) and plot any fieldline you desire.
'--Progam start---------
'Some Qbasic programs run very poorly under the control of Windows.
'ALT and ENTER toggles between screen modes. One of them should be OK.
'Control and Break breaks out of any Qbasic program.
'Anything preceded by the ' symbol is to be read as is.
'It's not part of the program.
'----------------------------------------------------------------------
ON TIMER(1) GOSUB tfix 'The next eight lines set the program
TIMER ON 'run speed to suit your computer.
WHILE stp < 10
pp = pp + 1
WEND
tfix:
ti = (pp / 10)
TIMER OFF
SCREEN 12: COLOR 9
LOCATE 28, 30: PRINT "Press any key."
COLOR 7: LOCATE 14, 1
PRINT " The purpose of the program is to demonstrate that a magnetic"
PRINT " field is nothing more than cycling electric fields."
DO: LOOP UNTIL INKEY$ <> ""
CLS
COLOR 7
LOCATE 1, 1
GOSUB cs
LOCATE 21, 25: PRINT "Transmitter. Receiver."
CIRCLE (250, 300), 4
CIRCLE (250, 300), 6
COLOR 12
LOCATE 10, 31: PRINT "+ +"
CIRCLE (250, 164), 4
CIRCLE (250, 164), 6
CIRCLE (354, 234), 4
CIRCLE (354, 234), 2
CIRCLE (346, 234), 4, 11
CIRCLE (346, 234), 2, 11
COLOR 11
LINE (250, 164)-(250, 300), 14
LINE (350, 164)-(350, 300), 14
LOCATE 28, 12
dd: FOR t = 1 TO ti: NEXT t
GOSUB ms
COLOR 11
LOCATE 20, 31: PRINT "- -"
CIRCLE (250, 300), 4
CIRCLE (250, 300), 6
COLOR 12
LOCATE 10, 31: PRINT "+ +"
CIRCLE (250, 164), 4
CIRCLE (250, 164), 6
FOR u = 1 TO 9: LINE (250 + (u * 10), 164)-(250 + (u * 10), 300), 11
LINE (250 - (u * 10), 164)-(250 - (u * 10), 300), 11
FOR t = 1 TO ti: NEXT t
GOSUB ms
LINE (250 + (u * 10), 164)-(250 + (u * 10), 300), 0
LINE (250 - (u * 10), 164)-(250 - (u * 10), 300), 0: NEXT u
CIRCLE (346, 234), 2, 0
CIRCLE (346, 234), 4, 0
CIRCLE (354, 234), 4, 0
CIRCLE (354, 234), 2, 0
CIRCLE (346, 230), 2, 11
CIRCLE (346, 230), 4, 11
CIRCLE (354, 238), 4, 12
CIRCLE (354, 238), 2, 12
FOR t = 1 TO ti: NEXT t
GOSUB ms
CIRCLE (346, 230), 2, 0
CIRCLE (346, 230), 4, 0
CIRCLE (354, 238), 4, 0
CIRCLE (354, 238), 2, 0
CIRCLE (346, 234), 2, 11
CIRCLE (346, 234), 4, 11
CIRCLE (354, 234), 4, 12
CIRCLE (354, 234), 2, 12
FOR t = 1 TO ti: NEXT t
GOSUB ms
COLOR 12
LOCATE 20, 31: PRINT "+ +"
CIRCLE (250, 300), 4
CIRCLE (250, 300), 6
COLOR 11
LOCATE 10, 31: PRINT "- -"
CIRCLE (250, 164), 4
CIRCLE (250, 164), 6
FOR u = 1 TO 9: LINE (250 + (u * 10), 164)-(250 + (u * 10), 300), 11
LINE (250 - (u * 10), 164)-(250 - (u * 10), 300), 11
FOR t = 1 TO ti: NEXT t
GOSUB ms
LINE (250 + (u * 10), 164)-(250 + (u * 10), 300), 0
LINE (250 - (u * 10), 164)-(250 - (u * 10), 300), 0: NEXT u
CIRCLE (346, 234), 2, 0
CIRCLE (346, 234), 4, 0
CIRCLE (354, 234), 4, 0
CIRCLE (354, 234), 2, 0
CIRCLE (346, 238), 2, 11
CIRCLE (346, 238), 4, 11
CIRCLE (354, 230), 4, 12
CIRCLE (354, 230), 2, 12
FOR t = 1 TO ti: NEXT t
GOSUB ms
CIRCLE (346, 238), 2, 0
CIRCLE (346, 238), 4, 0
CIRCLE (354, 230), 4, 0
CIRCLE (354, 230), 2, 0
CIRCLE (346, 234), 2, 11
CIRCLE (346, 234), 4, 11
CIRCLE (354, 234), 4, 12
CIRCLE (354, 234), 2, 12
GOTO dd
bc: LOCATE 1, 1: GOSUB cs
LOCATE 28, 30: PRINT "Press any key."
DO: LOOP UNTIL INKEY$ <> ""
LOCATE 1, 1: GOSUB cs
DO: LOOP UNTIL INKEY$ <> ""
CLS : GOTO bb
bb: COLOR 7
LOCATE 25, 1
PRINT " The flux lines of the field were plotted at steps"
PRINT " 80, 75, 70, 65, 60, 55, 50, 45, 40, 35, 30, 25, 20"
GOSUB ae
COLOR 7
LINE (270, 240)-(270, 340)
LINE (370, 240)-(370, 340)
ab: COLOR 7
LOCATE 23, 33: PRINT " "
LOCATE 24, 33: PRINT "100 50 0"
IF fld = 0 THEN LOCATE 1, 1: GOSUB cs
fld = fld + 1
IF fld < 2 THEN DO: LOOP UNTIL INKEY$ <> "": LOCATE 1, 1: GOSUB cs
COLOR 15: LOCATE 3, 12
IF fld > 1 THEN PRINT "Note: The white circle is the generated field line. "
IF fld > 1 THEN GOSUB xt
LOCATE 5, 10: INPUT "Enter field line point between conductors (1 to 100)"; a
IF a = 0 THEN CLS : GOSUB ae: GOSUB ak: GOTO ah
aa = a: ax = a: GOSUB am
LOCATE 24, 2: PRINT "Flux line origin ="; a
LINE (370 - ax, 450)-(370 - ax, 250)
GOSUB ag
LINE (270, 240)-(270, 400)
LINE (370, 240)-(370, 400)
c = 100 - a
b = c / a 'sets the ratio between the two conductors and the flux line
'reference point, which remains constant throughout the flux line.
aa: COLOR 7: LOCATE 24, 33: PRINT "100 50 0"
d = a * b: COLOR 10
IF c > 49.9 THEN CIRCLE (270, 230), d, (10), (3.1416 * 1.5), (3.1416 / 2)
IF c < 50.1 THEN CIRCLE (370, 230), a, (10), (3.1416 / 2), (3.1416 * 1.5)
COLOR 13
IF c < 50 THEN CIRCLE (270, 230), d
IF c > 50 THEN CIRCLE (370, 230), a
IF d > 100 + a OR a > 360 THEN GOTO ab
IF a > 100 + d OR d > 360 THEN GOTO ab
FOR t = 1 TO ti: NEXT t
IF c > 50 THEN COLOR 10
LOCATE 26, 2: PRINT "(a) Radius ="; d
COLOR 13
IF c < 50 THEN COLOR 10
LOCATE 27, 2: PRINT "(b) Radius ="; a
LOCATE 28, 4: PRINT "(a) / (b) ="; d / a; "(constant)"
a = a + 8
GOTO aa
ae: COLOR 14
CIRCLE (574, 230), 249
CIRCLE (450, 230), 120
CIRCLE (411, 230), 76
CIRCLE (393, 230), 53
CIRCLE (383, 230), 38
CIRCLE (377, 230), 27
CIRCLE (66, 230), 249
CIRCLE (190, 230), 120
CIRCLE (229, 230), 76
CIRCLE (247, 230), 53
CIRCLE (257, 230), 38
CIRCLE (263, 230), 27
LINE (320, 20)-(320, 380)
ag: COLOR 14
LINE (320, 20)-(320, 380)
COLOR 12
CIRCLE (270, 230), 4
CIRCLE (370, 230), 4
COLOR 13
CIRCLE (270, 230), 2
CIRCLE (370, 230), 2
RETURN
ak: COLOR 13
LINE (270, 230)-(370, 230)
CIRCLE (270, 230), 2
LINE (300, 120)-(300, 440), 15
CIRCLE (280, 230), 2
CIRCLE (290, 230), 2
CIRCLE (300, 230), 2, 15
CIRCLE (310, 230), 2
CIRCLE (320, 230), 2
CIRCLE (330, 230), 2
CIRCLE (340, 230), 2
CIRCLE (350, 230), 2
CIRCLE (360, 230), 2
CIRCLE (370, 230), 2
RETURN
cr: LOCATE 17, 1
cs: COLOR 7: READ rs$: PRINT " "; rs$
IF rs$ <> "" THEN GOTO cs
tp = tp + 1
IF tp = 4 THEN GOTO bc
IF tp = 10 THEN END
RETURN
ms: ss$ = INKEY$
LOCATE 28, 30: PRINT "Press any key."
IF ss$ <> "" THEN LOCATE 1, 1: GOSUB cs
RETURN
am: fa = 1: COLOR 15
cc = 100 - aa
bb = cc / aa
af: dd = aa * bb
IF dd > 100 + aa THEN CLS : CIRCLE (370 - ax + ((aa + ax) / 2), 230), (aa + ax) / 2: GOTO bm
IF aa > 6000 THEN CLS : GOTO bm
IF aa > 100 + dd THEN CLS : CIRCLE (270 + cc - ((cc + dd) / 2), 230), (cc + dd) / 2: GOTO bm
IF dd > 6000 THEN CLS : GOTO bm
aa = aa + 1
GOTO af
bm: RETURN
ah: COLOR 9
LOCATE 1, 28
PRINT "Press space bar to continue."
LOCATE 1, 1: COLOR 7
GOSUB cs
DO: LOOP UNTIL INKEY$ <> ""
GOSUB cs
xt:
LINE (270, 360)-(270, 368)
LINE (280, 360)-(280, 368)
LINE (290, 360)-(290, 368)
LINE (300, 360)-(300, 368)
LINE (310, 360)-(310, 368)
LINE (320, 360)-(320, 368)
LINE (330, 360)-(330, 368)
LINE (340, 360)-(340, 368)
LINE (350, 360)-(350, 368)
LINE (360, 360)-(360, 368)
LINE (370, 360)-(370, 368)
RETURN
DATA "The single pulse transmitter and the receiver are spaced far enough "
DATA "apart so that the static electric field is of little consequence. "
DATA " "
DATA "There is no doubt at all that the charges in the receiver will "
DATA "temporarily react to changes in the transmitter in exactly the "
DATA "manner indicated. There is also no doubt that the entire process, "
DATA "including the action of the magnetic field, is occurring in the "
DATA "plane of the dimension along which the charge relationship in the "
DATA "transmitter is changing. "
DATA ""
DATA "When the charge difference between the transmitter ends is at its "
DATA "maximum, for a short time the static electric field flux lines range "
DATA "between the greatest charge density of one sine to the greatest charge"
DATA "density of the opposite sine. A plot of equal charge density of one "
DATA "sine or the other can be found at any radius perpendicular to the axis"
DATA "of the electron movement along the transmitter length. And that's "
DATA "exactly where the strength of the magnetic field flux lines are found "
DATA "to be isotropic as well. They also are lines of equal intensity. "
DATA "In a sense, the two fields are identical. "
DATA ""
DATA "When electrons are flowing along the transmitter length in the process"
DATA "of inverting the charge on the ends, they are in motion relative to "
DATA "their fixed e+ counterparts. The electric field between every charge "
DATA "is being indexed along from one association to the next in line. The "
DATA "electric flux lines in a closer relationship with the action in the "
DATA "transmitter are indexed along at a greater rate, or more intense rate "
DATA "than the more distant flux lines. That action sets up rotation in much"
DATA "the same way as an air jet stirs the surrounding air mass. "
DATA " "
DATA " "
DATA ""
DATA "An analogy for magnetic attraction and repulsion can be taken from two"
DATA "air masses rotating in the same direction around the same point, in "
DATA "the same plane, while being driven from individual sources. But in "
DATA "this case, every molecule of each air mass is driven from its specific"
DATA "source drive. They will strongly resist any misalignment between the "
DATA "centers of rotation. Spin one air mass in the opposite direction and "
DATA "the two will be forced apart. "
DATA " "
DATA " "
DATA ""
DATA "From your viewpoint of the transmitter, when the charges are in the "
DATA "process of inverting to -- at the top and ++ at the bottom, the "
DATA "rotating electric field stirred into action by the more intense drive "
DATA "close to the transmitter body, is cycling anticlockwise on the left "
DATA "hand side of the transmitter body and clockwise on the right hand "
DATA "side. You see a south pole on the left and a north pole on the right. "
DATA "The two poles of a magnet are simply views of the same rotating "
DATA "electric fields taken from opposite directions. "
DATA " "
DATA " "
DATA " "
DATA " "
DATA " "
DATA ""
DATA " "
DATA " "
DATA " "
DATA "While the magnetic field is constant at any point along the "
DATA "transmitter, no current flow would be induced in either direction in a"
DATA "conductor that's moving around the transmitter axis at a constant "
DATA "radius about its centerline because the rotating electric-magnetic "
DATA "field remains isotropic throughout the motion. "
DATA " "
DATA " "
DATA " "
DATA " "
DATA " "
DATA ""
DATA "The flux lines in this image were generated by two, very long parallel"
DATA "conductors that are connected to form a closed loop circuit. The "
DATA "distance ratio between the two conductors and a specific point on any "
DATA "field line is exactly the same for every other point around that field"
DATA "line. "
DATA ""
DATA "Enter a point (1 to 100) between conductors to start a field line "
DATA "plot. Each set of circles intersect at a constant ratio between the "
DATA "point of intersection and the conductors. Or just press ENTER. "
DATA " "
DATA " "
DATA ""
DATA "Where the white line intersects the purple line drawn between the "
DATA "conductors, the distance ratio between the two conductors and that "
DATA "point is exactly the same when measured at any other point around "
DATA "the same flux line. "
DATA ""
DATA "When a constant current is flowing in an electromagnet coil, electric "
DATA "field change is occurring throughout the coil and the recording of "
DATA "each change MUST BE TRANSMITTED, but no matter what shape the coil "
DATA "is, the combined drive in any direction from the closed loop circuit "
DATA "arriving at any (stationary relative to the coil) point must always "
DATA "equal zero. The proof of this is in every magnetic field. One only "
DATA "needs to shift an appropriate detector across flux lines to see this "
DATA "proof (with eyes open of course). "
DATA ""
'---Program end--------