Hi T. A.,
Ah, thanks for the clarification! Now I understand what you're getting at.
Partial deflection does in fact happen during the time the control moves between the two extremes, but I'd say in practice this transition is rapid enough that we can neglect it for now. On the X-4, the two extremes aren't even neutral and full, but "opposite" and full.
The effective control force is however determined by the duty cycle. If the duty cycle is 60% "left", then the control will be deflected left 60% of the time and right 40% of the time.
Ignoring the rotation for the moment, if the missile were to follow the control input instantaneously, it would zigzag along on a sort of sawtooth curve, which leads the missile on a wide left turn, though 40% of the time it would be actually turning to the right. The individual segments of the zigzagging turn would be tight minimum radius turns.
Increase the duty cycle to 100%, and the missile would make a smooth and tight turn to the left. So even with the asuumption that the missile follows the controls without delay, you get different turn radii though the missiles zigzags around the desired path.
If we look at the missile in greater detail, it doesn't actually react to control inputs instantaneously. What actually happens is that the deflection of the control introduces a force that creates an angular acceleration of the missile. As the missile begins to increase its angle of attack, its main wings begin to ramp up a lift force that accelerate the missile in the commanded direction. The full (centripetal) lift force will only be reached after a delay, because it takes a while until the missile has rotated to the point where the equilibrium between control-induced force and stabilizing tailfin-induced force is reached.
This is basically a more extensive description of what Kramer itself described very briefly:
So if you have a 60% "left" duty cycle, the missile will probably oscillate from something like 50 % "left" to 70 % "left" angle of attack, and fly in a wide S-ing turn to the left, instead of the segemented tight-turn path from the "instantaneous" reaction model.
With the missile actually rotating about two times a second, all if this gets a bit more complicated as it happens in 3D, but the principles stay the same
I hope my explanation makes some sense at least? It's sort of difficult to describe without sketches, and I'm not very good at sketching, I'm afraid!
Regards,
Henning (HoHun)
I'll agree with the second, two axis control, but not with the first. You can't deflect a solenoid half way. It's on or it's off. That doesn't preclude rapidly banging it on and off, but you can't get partial deflection because solenoids don't work that way.
Ah, thanks for the clarification! Now I understand what you're getting at.
Partial deflection does in fact happen during the time the control moves between the two extremes, but I'd say in practice this transition is rapid enough that we can neglect it for now. On the X-4, the two extremes aren't even neutral and full, but "opposite" and full.
The effective control force is however determined by the duty cycle. If the duty cycle is 60% "left", then the control will be deflected left 60% of the time and right 40% of the time.
Ignoring the rotation for the moment, if the missile were to follow the control input instantaneously, it would zigzag along on a sort of sawtooth curve, which leads the missile on a wide left turn, though 40% of the time it would be actually turning to the right. The individual segments of the zigzagging turn would be tight minimum radius turns.
Increase the duty cycle to 100%, and the missile would make a smooth and tight turn to the left. So even with the asuumption that the missile follows the controls without delay, you get different turn radii though the missiles zigzags around the desired path.
If we look at the missile in greater detail, it doesn't actually react to control inputs instantaneously. What actually happens is that the deflection of the control introduces a force that creates an angular acceleration of the missile. As the missile begins to increase its angle of attack, its main wings begin to ramp up a lift force that accelerate the missile in the commanded direction. The full (centripetal) lift force will only be reached after a delay, because it takes a while until the missile has rotated to the point where the equilibrium between control-induced force and stabilizing tailfin-induced force is reached.
This is basically a more extensive description of what Kramer itself described very briefly:
"When the spoiler follows the varying pulses at sufficient frequency so that the inertia of the missile only permits the pulses to take effect according to their average, a simple yes-no control with full deflection has become, in the final result, a virtually proportional control without requiring any more effort."
So if you have a 60% "left" duty cycle, the missile will probably oscillate from something like 50 % "left" to 70 % "left" angle of attack, and fly in a wide S-ing turn to the left, instead of the segemented tight-turn path from the "instantaneous" reaction model.
With the missile actually rotating about two times a second, all if this gets a bit more complicated as it happens in 3D, but the principles stay the same
I hope my explanation makes some sense at least? It's sort of difficult to describe without sketches, and I'm not very good at sketching, I'm afraid!
Regards,
Henning (HoHun)