gar
Senior Member
- Location
- Ann Arbor, Michigan
- Occupation
- EE
120209-0959 EST
For clarification of what an is an oscilloscope I will describe a typical CRT (cathode ray tube) of the electrostatic deflection type.
The CRT has a more or less flat face coated with a phosphor that glows when and where an electron beam hits the screen. Internal to the tube there is a vacuum, thus nothing to obstruct electrons, an electron beam generator, and two sets of deflection plates perpendicular to each other.
The electron beam generator produces a very small diameter electron beam that is pointed toward the center of the screen. There are components in the electron beam generator to focus the beam to a small spot at the screen. Also there is a grid that can adjust the intensity of the beam and therefore the intensity of the spot on the screen. Thus, far there is just one small spot on the screen.
An electron beam passing thru an electrostatic field or magnetic field has its direction changed in proportion to that field intensity. Thus, if the beam is passed thru an adjustable electrostatic field (electric field, like in a capacitor), then the spot on the screen can be moved. If two sets of deflection plates are located inside the tube, but orientated so their electric fields are perpendicular to each other, then the spot on the screen can be positioned anywhere within some rectangular region on the screen.
With no amplifiers to confuse the issue we apply a sine wave from a single voltage source simultaneously to both sets of deflection plates the result is a Lissajous figure of a single straight line at 45 deg to horizontal. If the phasing of the signal to one set of plates is inverted (phase shift of 180 deg), then the angle of the straight line changes by 90 deg.
If the phasing of the two signals is 90 deg, then the result is a circle. Any other phase relationship produces an ellipse.
Next instead of placing a sine wave on the x-axis (typically horizontal) a linear sawtooth waveform is applied. Suppose its frequency is about 10 Hz, and not synchronized to anything, then in a linear fashion relative to time the beam moves from a point on the left side of the screen to a point on the right side in 1/10 second, and then immediately jumps back to the left side. Scopes are generally designed for increasing time going from left to right. What you see is a straight line of uniform brightness that is vertically in the middle of the screen.
Now apply to the y-axis (vertical) plates another signal. Make this signal a sawtooth of about 30 Hz. Now you see a sawtooth waveform on the on the screen of about 3 peaks and probably slowly drifting across the screen.
Change the horizontal sweep generator to one that can be synchronized to some other signal. This means make the starting point of its sweep start at a controlled point in time based on an external signal. Let that signal be the signal applied to the vertical axis and use the very rapid change of voltage of the y-axis sawtooth signal to be the trigger point. Now there will be exactly 3 saw teeth displayed on the screen without drift sideways.
Add a time delay from the trigger signal to when horizontal deflection starts and you can adjust the displayed starting point of the left side to any point on the vertical saw tooth.
Make the y-axis input a sine wave and the displayed waveform can start at any desired phase angle of the sine wave.
Thus, in the use of an oscilloscope to relate the phase of one signal to another it is important know what is the synchronizing signal and keep this a constant.
.
For clarification of what an is an oscilloscope I will describe a typical CRT (cathode ray tube) of the electrostatic deflection type.
The CRT has a more or less flat face coated with a phosphor that glows when and where an electron beam hits the screen. Internal to the tube there is a vacuum, thus nothing to obstruct electrons, an electron beam generator, and two sets of deflection plates perpendicular to each other.
The electron beam generator produces a very small diameter electron beam that is pointed toward the center of the screen. There are components in the electron beam generator to focus the beam to a small spot at the screen. Also there is a grid that can adjust the intensity of the beam and therefore the intensity of the spot on the screen. Thus, far there is just one small spot on the screen.
An electron beam passing thru an electrostatic field or magnetic field has its direction changed in proportion to that field intensity. Thus, if the beam is passed thru an adjustable electrostatic field (electric field, like in a capacitor), then the spot on the screen can be moved. If two sets of deflection plates are located inside the tube, but orientated so their electric fields are perpendicular to each other, then the spot on the screen can be positioned anywhere within some rectangular region on the screen.
With no amplifiers to confuse the issue we apply a sine wave from a single voltage source simultaneously to both sets of deflection plates the result is a Lissajous figure of a single straight line at 45 deg to horizontal. If the phasing of the signal to one set of plates is inverted (phase shift of 180 deg), then the angle of the straight line changes by 90 deg.
If the phasing of the two signals is 90 deg, then the result is a circle. Any other phase relationship produces an ellipse.
Next instead of placing a sine wave on the x-axis (typically horizontal) a linear sawtooth waveform is applied. Suppose its frequency is about 10 Hz, and not synchronized to anything, then in a linear fashion relative to time the beam moves from a point on the left side of the screen to a point on the right side in 1/10 second, and then immediately jumps back to the left side. Scopes are generally designed for increasing time going from left to right. What you see is a straight line of uniform brightness that is vertically in the middle of the screen.
Now apply to the y-axis (vertical) plates another signal. Make this signal a sawtooth of about 30 Hz. Now you see a sawtooth waveform on the on the screen of about 3 peaks and probably slowly drifting across the screen.
Change the horizontal sweep generator to one that can be synchronized to some other signal. This means make the starting point of its sweep start at a controlled point in time based on an external signal. Let that signal be the signal applied to the vertical axis and use the very rapid change of voltage of the y-axis sawtooth signal to be the trigger point. Now there will be exactly 3 saw teeth displayed on the screen without drift sideways.
Add a time delay from the trigger signal to when horizontal deflection starts and you can adjust the displayed starting point of the left side to any point on the vertical saw tooth.
Make the y-axis input a sine wave and the displayed waveform can start at any desired phase angle of the sine wave.
Thus, in the use of an oscilloscope to relate the phase of one signal to another it is important know what is the synchronizing signal and keep this a constant.
.