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CLAUDE.md
148
CLAUDE.md
@@ -41,8 +41,6 @@ Use // for single line comments
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use /* */ for multiple block comments spanning multiple lines
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avoid using auto
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_______________________________________________________
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Summary of project:
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This is a museum exhibit displaying and providing interaction
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@@ -53,16 +51,152 @@ radars in that era. The different radars are:
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Scopes in the right panel
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1. A-scope for Chain Home Radar in the 1940's (first radar and could be tricky)
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2. A-scope for marine radar in the 1950's (Before PPI radar. Was a bit tedious to operate
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2. A-scope for marine radar in the 1950's (Before PPI radar); was a bit tedious to operate
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3. PPI scope for marine traffic control (uses beam sweeping in all 360 degrees of
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rotation; Easier to use than a scope
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rotation); Easier to use than a scope
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4. PPI scope for air traffic control; similar to PPI scope for marine, but with different range
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5. PPI scope on board a boat. Shows how movement of a boat affects the radar display
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6. Precision Approach Radar (Two scopes; one showing horizontal movement of a plane
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in the glide path toward the runway, and the other showing vertical movement of a plane
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as it glides vertically down to the runway.
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as it glides vertically down to the runway). Both scopes will be seen if this is selected.
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Text window in the left panel for descriptions of the scopes and a listing of controls
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Please note that these scopes will not appear all at once. The selection of which scope
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the visitor sees is done by pressing a forward control and a reverse control to go around
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the loop of scopes.
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Also, please note that the state of the controls of each scope is independent of any
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other scope. Furthermore, the controls will reset when a scope is exited and then re-entered.
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The Text window in the left panel for descriptions of the scopes and a listing of controls
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Controls to affect the behavior of the scopes; (these first implemented using keyboard
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strokes; later when physical controls are completed, the keyboard controls will be removed.
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strokes; later when physical controls are completed, the keyboard controls will be removed)
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The controls will affect state variables that will be sent to the shaders as uniforms.
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There will be three abstracts for scopes:
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1. A Scope - sweep on horizontal axis. A pulse will appear for a return. The distance from
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the left hand side to the pulse is the range. The height of the pulse is the strength
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of the return signal. The bearing is determined by manual control.
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The basic controls for both A Scopes include:
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Intensity (the overall brightness of the entire display).
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Sensitivity (the strength of the signal amplification of the
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receiver). This has nothing to do with the brightness of the
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pulses. This only affects the height of the pulse and the height
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of any noise floor.
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Chain Home A Scope
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Because the receiving antennas are very large (about 100 feet), the
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operator cannot physically move them.
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Therefore, the bearing is determined through a process called radio direction
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finding (RDF) using a specialized instrument known as a Radiogoniometer.
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The receiver towers (which were separate from the transmitter towers)
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featured two sets of dipole antennas mounted at right angles to one
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another—essentially one oriented North-South and the other East-West.
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The signals from these two perpendicular antennas were fed into a Radiogoniometer
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located in the receiver hut. Inside the device there are two fixed coils (field coils)
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that were mounted at right angles matching the orientation of the outdoor antennas.
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A third coil, the search coil, is mounted on a rotating shaft inside the two
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field coils. The operator would physically turn a knob to rotate the search coil.
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The relative strength of the signal in each antenna depended on the angle of the
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incoming wave. For example, a target directly to the North would produce a maximum
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signal in the North-South antenna and zero in the East-West antenna.
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The operator would look for a null point (a signal or pip weaker than the noise floor).
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At that point, the operator would read the bearing from a calibrated scale attached
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to the radiogoniometer knob.
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We can simulate the radiogoniometer knob that would affect the null point depending
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on the bearing of a target. The museum visitor could experience seeing different
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null points for each target. Since we do not have a physical calibrated knob, we
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can put the bearing as a text indicator below the A Scope.
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The range is 200 miles.
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There is also a selection for the pulse repetition frequency (PRF). A switch was
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used to select one of two PRFs. One is 50 pulses per second and the other is 25
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pulses per second. This selection should also be indicated in the status text
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below the scope. We need to have a keyboard selection to cycle this selection
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as well as a switch on the control panel.
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There is a glass or plastic graticule that is etched with vertical lines
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representing range. This is edge-lit with incandescent lamps.
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Because of natural drift of period electronic components, they needed an
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electronic calibration, or strobe.
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This is a crystal oscillator which is
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steady and precise.
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The pip generated by this circuit can be moved via knob or keyboard keys and
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its position is indicated on the text status line below the scope.
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The operator aligns this pip with a target pip in order to get an accurate
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range to the target.
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Marine A Scope
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Marine radar frequencies allowed the use of much smaller antennas;
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dishes or horns. Those antennas would be mounted on the shaft of a servo motor. The
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servo motor would be driven by another servo that is attached to the bearing control
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knob on the radar console. The bearing is on a calibrated dial on the bearing control
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knob.
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We can simulate the bearing knob that would affect the simulated pointing of the
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dish antenna. The museum visitor could experience seeing different
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pips appear as they rotate the antenna toward them. Likewise the pips would disappear
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as the antenna is rotated away.
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The range is indicated at how far the pip is from the left hand side of the scope which
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is the location of the radar transmitter. If the target goes further away,
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the pip will move to the right. If the target comes close to you, the pip will
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move left.
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This pip has a finite rise time as the transmitter starts.
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The width is set by the modulator stage in the transmitter.
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Following the width, the pip has a finite fall time as the transmitter stops. This
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creates a curved waveform; not just a line.
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Here is some information on the pulse width for these old A Scope Marine Radars. There is
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a switch that selects two pulse widths. Option 1 is Short Pulse (0.1 microsecond) for harbor
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navigation and Option 2 is Long Pulse (1 microsecond) for open sea detection. We need
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to implement this control. Perhaps a single keyboard key or single physical button.
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Range and range lines on graticule
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Please note that the graticules are plastic overlays over the screen. They need to be removed
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and replaced when the operator changes the maximum range. This can be simulated with the graticule
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being lifted toward the top of the scope as it is removed. Then the new graticule would be slid
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down until it covers the scope. The graticule will be edge-lit with an incandescent lamp.
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Here is a table of the available ranges and what markings will be on the plastic graticule.
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1. 1.5 miles; markers every 0.25 miles
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2. 3.0 miles; markers every 0.5 miles
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3. 6.0 miles; markers every 1.0 miles
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4. 12.0 miles; markers every 2.0 miles
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There would be four available plastic overlays.
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Range can be selected with two keyboard keys or two buttons on the panel, and is
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indicated in the text status panel below the scope.
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Please note that the range setting and the pulse width are separate controls.
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There are two reasons.
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1. Target discrimination and detection. Short pulse results in better range resolution while
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a longer pulse width results in better detection of distant and weak targets.
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2. Magnetron Duty Cycle. Too much time with long pulse width can put a strain
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on the magnetron.
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2. PPI Scope - still being worked
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3. PAR Scope - still being worked
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