Summary: Two videos of similar (perhaps the same) objects over coastal Israel, appear to show characteristics that are commonly associated with UFOs; erratic motion, an amazing range of speeds, and right angle turns. The most unusual characteristic is what appears to be erratic motion; although the object size is unknown, conservative estimates of the object size, result in object accelerations that are not feasible with known technology, and would probably destroy any known aircraft. Like most videos, the cameras are zoomed, leaving out terrestrial objects that would be used as reference points to determine UFO motion. Fortunately, the cameras were able to see background stars, making the measurement of UFO motion possible. Report: On the evening of July 22, 1999, over the Israeli "Special" (nuclear?) Air Force Base at Palmachim-Yavne (S. of Tel Aviv), an object was reported to fly from the north to the coastal area where it stopped and hovered above the base. No noise was reported in the six hours the object hovered. Over 100 witnesses reportedly saw the object; several are seen on the video submitted. Planes were reported circling the object at a distance, although none appear on video. The video was about 12 minutes long; the tape has gaps, and with no onscreen time, the actual duration covered is unknown. Generally, the video shows the camera zooming into the object, giving extreme magnification. The camera is capable of digital zoom, which mostly provides magnification and artifacts but no true detail. When normal hand-holding jiggle causes the object to be lost, the camera is fully de-zoomed, the object relocated, and zooming reattempted. This allows intermittent views of the object position in the sky (compared with streetlight positions), alternated with views of the object shape. The composite image Fig. 1 shows the object position at the noted time in seconds from the beginning of the video. Note the non-linear path of the object. Also note that the object moves a considerable angular distance in about a minute. (A witness face is obscured for privacy.) In close zooms, the object shows a wide variety of shapes. The composite Fig. 2 shows some of those seen. None of these images are "one-frame-wonders"; all shapes shown are visible in numerous frames, and are therefore not merely due to random tape noise or other intermittent artifacts. Equally important is to recognize what is NOT "seen" (video artifacts as opposed to real images). The horizontal and vertical lines are camera artifacts of digital zoom and interlace, and should not be taken as actual structure of the object. Relative brightnesses of light are valid data, taking overexposure into account. The actual colors of small objects are not properly recorded onto videotape, due to video bandwidth limitations. A bright overexposed object appears white, regardless of actual color. A large blob should not be taken as a true size, this usually indicates imperfect focus of the camera. A bright area around a white light, fading with distance from center, is probably glare. As the glare is often not overexposed and is over a large area, its color is indicative of the actual object's color, even if overexposed. Click here for negative video of UFO Most camcorders will detect near infrared, in the range of 700- 1000nM (nanometers wavelength). For reference, the human eye sees violet near 400nM, up to red near 700nM. Silicon photodetectors, the usual heart of a camcorder video signal, typically have peak response around 700nM, near infrared. A camcorder infrared response can be tested by looking at a TV remote control through the camera while pushing buttons on the remote; infrared response will be seen as white flashes in the camera that can't be seen by eye. Infrared in a video can be distinguished in three ways: It will be seen though the camera, but not by the naked eye (if excited witnesses take care to note!); it appears white; and being a longer wavelength, will focus differently. "Near infrared" should be distinguished from "thermal infrared" which is a far longer wavelength not detectable by ordinary camcorders, often used in night-vision equipment. For a typical achromatic lens, infrared underfocuses; it is bent less, so the lens-image distance must be greater than for visible light. The result can be a ring shape, distinct from properly focussed, visible light images in the same scene. Note: The object typically shows two or three lights, sometimes with one or two dimmer lights. The bright/dim distinction changes; in one segment, an equilateral triangle arrangement slowly turns counter-clockwise and flattening, with the lower left light dimming until the object resembles a pair of lights with a dimmer light between. It should be noted that the characteristic flash of airplane anti-collision strobe lights are never seen in the video. Note: In the 5th image down in Fig. 2, the appearance of a "headphones" shape. The "headstrap" bridging the "earphones" is not a segment of a circle, indicating merely a mis-focused point of light. The aspect ratio (height/width ratio) is about 1.5/1, clearly different than a circle. During the headstrap's visibility, occasional twinkles are seen within it; it appears to be a real object, not an artifact. The 6th to 8th images in Fig. 2 show a ring of light. Particularly in the 8th frame, the "earphones" are in fairly good focus but the ring is quite evident. This would be consistent with a strong infrared source, producing an under-focused ring image, while visible wavelengths are in proper focus. The images in Fig. 3, the result of digital zoom, are useful with the repeated caveat that the vertical pattern is from digital zoom, not a real attribute of the object. The uppermost frame shows the right light extremely over-exposed, showing an orange result in the non over-exposed glare. This orange result should be interpreted with caution; even the best cameras produce poor color at night. Note in your local nightly weather forecast, live camera shots of city interstate intersections may be shown for gauging traffic or weather. The picture will appear quite red, although any driver knows the scene is yellowish-white. This is due to the sodium-yellow lights' wavelength registering on the red channel of the camera. The true color could be yellower than what is seen on the video. The important aspect of this image is that the object has an extremely bright yellow/orange light, with two much weaker white lights. This combination is inconsistent with typical aircraft lighting; extremely bright lights are typically landing lights, which are white. The last three images in Fig. 3 show closeups of a three-light arrangement, with the lower two lights in fairly sharp focus (although much glare) but the upper light in very bad focus. The difference between glare and focus is obvious; the lower circles have an clear source in the bright centers, but the upper ring has little or no distinguishing center. This verifies the upper ring is the result of poor focus of that wavelength, not glare. As the other points are in fairly good focus, the mis-focus is apparently due to a wavelength difference between the lower lights and the upper. Infrared light appears to be the only candidate which would cause this result; ultraviolet light penetrates glass poorly and registers on silicon photoreceptors poorly.
At several points in closeups in the video, persistent points of light (as opposed to random spots of video noise) appear in the same, or at least in predictably different, positions on the screen. This is consistent with a background star (example in Fig. 4, circled) appearing in the video, appearing to bounce around due to the unsteadiness of the videographer's hand. (I could not find a weather report verifying clear skies that night; another source of light, such as a plane running light, gives little change in the conclusions so based.) Such a reference star is very useful in that it can be used to determine the true angular motion of the object, as long as the object is far enough away that positional movement of the camera generates no significant parallax error. Given the numerous witnesses referring to a distant object, and the degree of zoom making any significant lateral movement of the camera difficult while maintaining aim, the possibility of parallax seems doubtful for giving a significant apparent shift between the star and the object. The results shown below, therefore, appear to be true angular motion of the object rather than the result of artifacts. Shown, graphically in Fig. 5, is the X-difference (solid line with square markers, in units of screen pixels on a 640-by-480 display) and Y-difference (thick line) between the object and the star over a 145-frame time period (almost five seconds). As a size reference, the object is about 40 pixels wide center-to-center of its outermost lights. The X-difference between the star and the camera aim is shown as a dotted line with triangle markers. The star is often not clearly visible, being smeared out by camera motion to obscurity or simply off screen. Such points are unmarked on the graph. Note: The object made five reversals in direction in these five seconds - an astonishing performance. The maximum lateral motion is about six times the apparent width of the object. Assuming (as a probably conservative guess - see below) that the object is 10 feet across, the object went 60 feet back and forth in about 1 second. The maximum acceleration is about 18G. This is consistent historically with witness reports in which erratic UFO flight is reported, and quite uncharacteristic with known aircraft performance. The reference star does not appear to be a lens flare from any of the numerous street lights in the area (or of the object itself). Several lens flares ARE obvious during low-zoom conditions. If a lens flare, it would have the shape (perhaps reflected and/or inverted) of the source light; instead, the star is small and point-like. But, assuming the object to be motionless, and that the apparent motion is totally camera motion, the "star" motion should correlate to the camera motion. This is since a lens flare is merely a reflection off some stray surface inside the lens, and moving the "mirror" (lens/camera) will also move the reflection accordingly. But no such correlation is found. All indications are that the star is a distant point-like object, and a valid reference point. The graph in Fig. 6 shows another segment of the video where a star appeared useful as a reference point, with the same symbology as the previous graph. Similarly, about 8 reversals are seen in about a seven second period. The object width is about 60 pixels, so the object moved laterally about six times its own width back and forth. Near the end of the segment, extreme motion of the camera smeared out the star image beyond recognizability, so this portion of the graph is blank. Extreme motion of the camera can be useful. The image in Fig. 7 shows a streak generated, presumably when the camera was bumped; the previous frames are also disturbed as if bumped. The streak shows a time exposure of the object during the 1/50 second exposure of a single field. The brightness of the streak is representative of the brightness times the duration the light spent at a particular point on the image. Since the motion of the camera isn't known, the time duration during the streak is not known. However, since there are two lights, IF the lights are of constant brightness, one would expect the brightnesses of the two treaks to correspond; a bright region of one light's streak would correspond to a bright region of the other. This effect is not seen; corresponding parts of the two streaks are obviously of different brightness. The differing brightnesses could be explained by several phenomenon, all resulting in an anomalous conclusion: 1. The lights are rapidly changing brightness. Standard tungsten aircraft lights are incapable of doing this. 2. Atmospheric turbulence (twinkling) is causing the brightness changes. This implies a considerable amount of air between the object and camera; the amount depends on distance and the air stability. A hot night will have more thermal action than a cold still night. (A large amount of heat roiling off the object, such as looking directly into a jet exhaust, will also cause turbulence.) Assuming no object heat, I would guess at least several kilometers of air between the object and camera to generate this amount of twinkling. Conservatively assuming one kilometer distance, and 100X digital zoom (which is a guess, but typical) and a pair of lights 1/3 of the frame-width, the light spacing is 1000 meters / 100X zoom * 1/3, or about 3 meters apart. Often, three or more lights at similar spacings are seen, so the object size is at least twice this size.
In both graphs, the camera motion clearly lags the object motion by about 1/3 second; this is what would be expected of a videographer trying to "track" an erratically moving object. The 1/3 second delay is what would be expected from studies of computer mouse and trackball human response testing, and also is on the slow end of TV cameramen's performance in tracking the football during unexpected events (intercepts, fumbles, fake handoffs, etc.) during NFL play. So the camera motion is quite typical of what would be expected from normal human hand-eye coordination. This is also additional confirmation that the star is not simply a lens flare; a lens flare's position would react instantly to camera motion, not with a delay. A summary of the object characteristics: 1. No standard aircraft anti-collision strobes are ever seen. 2. The object path is atypical for a plane. A helicopter could easily make such a path, although hovering silently for six hours is a gas-guzzling challenge. 3. The arrangement of lights changes continuously, often assuming a non-horizontal arrangement. Airplanes, unless viewed from substantially below, appear as inherently horizontal objects. 4. A "headstrap" structure is seen which appears to be real, and does not match any lighted airplane or helicopter structure I am familiar with. 5. At one point, the object's brightest light, by far, is approx. orange (perhaps yellow or red). An extremely bright light of this color is not standard on any airplane I am familiar with. 6. At another point, the object appears to have a light source that emits infrared (approximately 900nM) with little or no corresponding visible light. 7. The object position, compared to reference stars, is erratic. Although the object size is unknown, even conservative size estimates yield astonishing acceleration results. The first six characteristics might be achieved with a determined faker with an incredible helicopter and a complex array of visible and infrared lights, but the last characteristic is implausible for any known aircraft. On the evening of September 2, 1998, a 14 minute videotape was recorded showing a similar strange triangle of lights, described as red/yellow/blue, "patrolling the skies of Rishon Leziyon" (sometimes translated as Le Zion or Letzion) on coastal Israel. The camcorder is obviously handheld, with the usual shakiness of a handhold with zoom. The zoom varies, showing perhaps 16X zoom alternated with occasional shots of a crowd of onlookers. Not surprisingly due to the limited ability of videotape to capture the color of small objects, no color other than a slight pink was detected. The triangular array slowly turns clockwise, with lights occasionally extinguishing, and being replaced with lights on the opposite side. Figure 8 shows a collection of images of the object, with timing information. The on-screen time is shown where available; if not, the frame number is given. Apparent size changes are presumably due to zoom changes. The last image is that of an airplane; the center bright light is an anti-collision strobe light.
The graph in Fig. 9 below shows the turning of the lights. Note the object appears to make about 1.5 complete revolutions. The turning is accomplished in slow turning, then bursts, both of which slow during the video. After 150 seconds, the time is real time as shown by the camcorder on-screen time display. Prior to 150 seconds, the time is estimated assuming the camcorder ran continuously. This is not true; there are breaks of unknown duration in the video. Timing prior to 150 seconds should be regarded as speculative. Note also that the time covered is longer than the video length; this is due to breaks in the recording. Several frames show smearing of the light images due to camera motion. No interesting high speed brightness changes were apparent in such frames. At several portions of the video, background stars appear to be visible (circled at right). These are very useful in that true object motion is apparent using the star as a reference point. (In the portion shown, two stars are visible, allowing a zoom change to be compensated for. In this and another brief segment where two stars are visible, they are motionless relative to each other, corroborating the conclusion that these points are indeed stars.) These portions are: At 30 seconds, over 42 frames (8 points measured, although many more visible), object moves leftward and downward at a 45 degree angle, at a speed of 2.5 times its own length per second. At 97 seconds, over 32 frames (but only 3 frames showed a star), object moves right and upward at a 70 degree angle at a speed of 7X its own length per second. At 124 seconds, over 21 frames (but only 3 frames showed a star), object moves rightward and downward at a 25 degree angle, at a speed of 9X its own length per second. At 164 seconds, at 18:38:35, over 86 frames (9 measured), object left and down at a 40 degree angle at a speed of 2X its own length per second. At 18:40:04, over 225 frames (18 measured with 2 stars), object right and down at a 17 degree angle at a speed of 6X its own length per second. At 18:45:45, over 31 frames (only 3 measured), object right and upward at a 28 degree angle at a speed of 11X its own length per second. At 18:49:24, over 67 frames (7 measured), object right and upward at a 14 degree angle at a speed of 13X its own length per second. At 18:52:36, over 333 frames, (9 points measured using 2 stars) rightward and upward at a 44 degree angle, at about 1.4 times its own length per second. At 18:59:44, over 211 frames, (7 measured) leftward and upward at a 48 degree angle, at a speed of about 0.8X its own length per second. "Its own length" refers to the maximum distance between lights; the size of a possible dark supporting structure is obviously unknown. "Frames" are the 1/30 second NTSC frames studied, although the original PAL video is recorded at 25FPS. In all cases, the object motion was a straight line over all measured intervals, within measurement error limits. Note that faster speeds correspond to fewer data points. As would be expected in the case of high object speed, only a small number of samples could be obtained before the star left the field of view. Also, fast motion smears out and obscures a dim object, making a star harder to find. The variety of directions and speeds may be better understood by looking at the series of lines in Fig. 10; the direction of each arrow shows the direction of the object, and the length of the lines represents the object speed. Note, THE LENGTH OF THE LINE DOES NOT REPRESENT THE ACTUAL PATH OF THE OBJECT, but rather its speed at the stated times. In summary, the description of "patrolling" is corroborated; between 30 and 97 seconds, the object turned almost completely around, turned right, down slow, right, up fast, then slowed and turned left. Note the number of near-right-angle turns. OTHER TURNS (WITH NO STAR AS REFERENCE) MAY HAVE OCCURRED. Remember this motion is apparent motion; the object could be moving toward or away from the camera and this motion would not be visible. Conclusion: The object is obviously not an airplane, or some device on an airplane; ignoring the lack of standard lighting, the path, and the 16:1 range of apparent speed, is impossible. A turnable set of lights on a helicopter could make this video, but I doubt that numerous witnesses would fail to recognize helicopter noise. A helicopter would have particular difficulty making a 1 minute, 180 degree turn silently. I know of no known cause for this phenomenon. Jeff Sainio MUFON Staff Photoanalyst 7206 W. Wabash Ave. Milwaukee, WI 53223-2609