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Slot liner

slot liner

Englisch-Deutsch Übersetzung für slot liner und Beispielübersetzungen aus technischen Dokumentationen. Nutauskleidung, Drahtführung, Steckplatz, Schlit.. . Übersetzung im Kontext von „the slot liner“ in Englisch-Deutsch von Reverso Context: A rotor according to claim 7, wherein said slot armor halves () are. Lernen Sie die Übersetzung für 'liner slot' in LEOs Englisch ⇔ Deutsch Wörterbuch. Mit Flexionstabellen der verschiedenen Fälle und Zeiten ✓ Aussprache und.

Their main drawback is that they are labour-intensive to use and require calculation, tables, or plotting to make use of the results. They need to be made with mechanical precision and the probe and its detector need to be adjusted with care, but they can give very accurate results.

The slotted line is one of the basic instruments used in radio frequency test and measurement at microwave frequencies.

It consists of a precision transmission line , usually co-axial but waveguide implementations are also used, with a movable insulated probe inserted into a longitudinal slot cut into the line.

In a co-axial slotted line, the slot is cut into the outer conductor of the line. The probe is inserted past the outer conductor, but not so far that it touches the inner conductor.

In a rectangular waveguide, the slot is usually cut along the centre of the broad wall of the waveguide. Circular waveguide slotted lines are also possible.

Slotted lines are relatively cheap [note 1] and can perform many of the measurements done by more expensive equipment such as network analysers.

However, slotted line measurement techniques are more labour-intensive and often do not directly output the desired parameter; some calculation or plotting is frequently required.

In particular, they can only carry out a measurement at one spot frequency at a time so producing a plot of a parameter versus frequency is very time consuming.

This is to be compared to modern instruments like network and spectrum analysers which are intrinsically frequency swept and produce a plot instantly.

Slotted lines have now largely been superseded, but are still found where capital costs are an issue. Their remaining uses are mostly in the millimetre band , where modern test apparatus is either prohibitively expensive or not available at all, and with academic laboratories and hobbyists.

They are also useful as a teaching aid as the user is more directly exposed to basic line phenomena than with more sophisticated instruments.

The slotted line works by sampling the electric field inside the transmission line with the probe. For accuracy, it is important that the probe disturbs the field as little as possible.

For this reason the probe diameter and slot width are kept small usually around 1 mm and the probe is inserted in no further than necessary.

It is also necessary in waveguide slotted lines to place the slot at a position where the current in the waveguide walls is parallel to the slot.

The current will then not be disturbed by the presence of the slot as long as it is not too wide. For the dominant mode this is on the centre-line of the broad face of the waveguide, but for some other modes it may need to be off-centre.

This is not an issue for the co-axial line because this operates in the TEM transverse electromagnetic mode and hence the current is everywhere parallel to the slot.

The slot may be tapered at its ends to avoid discontinuities causing reflections. The disturbance to the field inside the line caused by the insertion of the probe is minimised as far as possible.

There are two parts to this disturbance. The first part is due to the power the probe has extracted from the line and manifests as a lumped equivalent circuit of a resistor.

This is minimised by limiting the distance the probe is inserted into the line so that only enough power is extracted for the detector to operate effectively.

The second part of the disturbance is due to energy stored in the field around the probe and manifests as a lumped equivalent of a capacitor.

This capacitance can be cancelled out with an inductance of equal and opposite impedance. Lumped inductors are not practical at microwave frequencies; instead, an adjustable stub with an inductive equivalent circuit is used to "tune out" the probe capacitance.

The result is an equivalent circuit of a high impedance in shunt across the line which has little effect on the transmitted power in the line.

The probe is more sensitive as a result of this tuning and the distance it is inserted can be further limited as a result. A typical test setup with a waveguide slotted line is shown in figure 2.

Referring to this figure, power from a test equipment source not shown enters the apparatus through the co-axial cable on the left and is converted to waveguide format by means of a launcher 1.

This is followed by a section of waveguide 2 providing a transition to a smaller size of guide. An important component in the setup is the isolator 3 which prevents power being reflected back into the source.

Depending on the test conditions, such reflections can be large and a high-power source may be damaged by the returning wave.

The power entering the slotted line is controlled by a rotary variable attenuator 4. This is followed by the slotted line itself 5 above which is the probe mounted on a movable carriage.

The carriage also carries the probe adjustements: The load can be replaced by the component or system that it is desired to test.

It can also be replaced with a reference short-circuit 10 which is used to calibrate the slotted line. The carriage can be moved along the slotted line by means of a rotary knob 11 which simultaneously moves a vernier gauge 12 for accurate measurement of the probes position along the line.

The probe is connected to a detector and a display meter not shown in figure 2. These can be, respectively, a thermistor and power meter, or an envelope detector and VSWR meter.

The detector can be a crystal detector or a Schottky barrier diode. This is because the detector looks almost like a short circuit to the transmission line, and this distance will convert it to an open circuit through the quarter-wave impedance transformer effect.

Thus, the detector has minimal effect on loading the line. The probe tuning stub can be seen on figure 3 branching from the line linking the probe to the detector.

Figure 2 has a slightly different arrangement; the main probe into the waveguide leads to a vertical co-axial tuning and adjustment section but the detector is on a horizontal side-section with a secondary probe into the upright co-axial section.

Measurements of microwave power can be made directly, usually with a thermistor based detector and meter. However, these instruments are expensive and a common meter used in measurements with a slotted line is instead a cheaper low-frequency VSWR meter.

The microwave power source is amplitude modulated with, typically, a 1 kHz signal which is recovered by the envelope detector in the probe and sent to the VSWR meter.

This scheme is preferred to simply detecting the unmodulated carrier directly, which would result in a DC output, because a stable, narrowband, tuned amplifier can be used to amplify the 1 kHz signal.

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It consists of a precision transmission line , usually co-axial but waveguide implementations are also used, with a movable insulated probe inserted into a longitudinal slot cut into the line.

In a co-axial slotted line, the slot is cut into the outer conductor of the line. The probe is inserted past the outer conductor, but not so far that it touches the inner conductor.

In a rectangular waveguide, the slot is usually cut along the centre of the broad wall of the waveguide. Circular waveguide slotted lines are also possible.

Slotted lines are relatively cheap [note 1] and can perform many of the measurements done by more expensive equipment such as network analysers.

However, slotted line measurement techniques are more labour-intensive and often do not directly output the desired parameter; some calculation or plotting is frequently required.

In particular, they can only carry out a measurement at one spot frequency at a time so producing a plot of a parameter versus frequency is very time consuming.

This is to be compared to modern instruments like network and spectrum analysers which are intrinsically frequency swept and produce a plot instantly.

Slotted lines have now largely been superseded, but are still found where capital costs are an issue. Their remaining uses are mostly in the millimetre band , where modern test apparatus is either prohibitively expensive or not available at all, and with academic laboratories and hobbyists.

They are also useful as a teaching aid as the user is more directly exposed to basic line phenomena than with more sophisticated instruments.

The slotted line works by sampling the electric field inside the transmission line with the probe. For accuracy, it is important that the probe disturbs the field as little as possible.

For this reason the probe diameter and slot width are kept small usually around 1 mm and the probe is inserted in no further than necessary.

It is also necessary in waveguide slotted lines to place the slot at a position where the current in the waveguide walls is parallel to the slot.

The current will then not be disturbed by the presence of the slot as long as it is not too wide. For the dominant mode this is on the centre-line of the broad face of the waveguide, but for some other modes it may need to be off-centre.

This is not an issue for the co-axial line because this operates in the TEM transverse electromagnetic mode and hence the current is everywhere parallel to the slot.

The slot may be tapered at its ends to avoid discontinuities causing reflections. The disturbance to the field inside the line caused by the insertion of the probe is minimised as far as possible.

There are two parts to this disturbance. The first part is due to the power the probe has extracted from the line and manifests as a lumped equivalent circuit of a resistor.

This is minimised by limiting the distance the probe is inserted into the line so that only enough power is extracted for the detector to operate effectively.

The second part of the disturbance is due to energy stored in the field around the probe and manifests as a lumped equivalent of a capacitor.

This capacitance can be cancelled out with an inductance of equal and opposite impedance. Lumped inductors are not practical at microwave frequencies; instead, an adjustable stub with an inductive equivalent circuit is used to "tune out" the probe capacitance.

The result is an equivalent circuit of a high impedance in shunt across the line which has little effect on the transmitted power in the line.

The probe is more sensitive as a result of this tuning and the distance it is inserted can be further limited as a result.

A typical test setup with a waveguide slotted line is shown in figure 2. Referring to this figure, power from a test equipment source not shown enters the apparatus through the co-axial cable on the left and is converted to waveguide format by means of a launcher 1.

This is followed by a section of waveguide 2 providing a transition to a smaller size of guide. An important component in the setup is the isolator 3 which prevents power being reflected back into the source.

Depending on the test conditions, such reflections can be large and a high-power source may be damaged by the returning wave.

The power entering the slotted line is controlled by a rotary variable attenuator 4. This is followed by the slotted line itself 5 above which is the probe mounted on a movable carriage.

The carriage also carries the probe adjustements: The load can be replaced by the component or system that it is desired to test.

It can also be replaced with a reference short-circuit 10 which is used to calibrate the slotted line. The carriage can be moved along the slotted line by means of a rotary knob 11 which simultaneously moves a vernier gauge 12 for accurate measurement of the probes position along the line.

The probe is connected to a detector and a display meter not shown in figure 2. These can be, respectively, a thermistor and power meter, or an envelope detector and VSWR meter.

The detector can be a crystal detector or a Schottky barrier diode. This is because the detector looks almost like a short circuit to the transmission line, and this distance will convert it to an open circuit through the quarter-wave impedance transformer effect.

Thus, the detector has minimal effect on loading the line. The probe tuning stub can be seen on figure 3 branching from the line linking the probe to the detector.

Figure 2 has a slightly different arrangement; the main probe into the waveguide leads to a vertical co-axial tuning and adjustment section but the detector is on a horizontal side-section with a secondary probe into the upright co-axial section.

Measurements of microwave power can be made directly, usually with a thermistor based detector and meter.

However, these instruments are expensive and a common meter used in measurements with a slotted line is instead a cheaper low-frequency VSWR meter.

The microwave power source is amplitude modulated with, typically, a 1 kHz signal which is recovered by the envelope detector in the probe and sent to the VSWR meter.

This scheme is preferred to simply detecting the unmodulated carrier directly, which would result in a DC output, because a stable, narrowband, tuned amplifier can be used to amplify the 1 kHz signal.

When the slotted line is terminated with a precision matching load there is no variation in the detected power along the line, other than a very small decrease due to losses in the line.

However, when this is replaced by a device under test DUT which is not perfectly matched to the line there will be a reflection back towards the source.

This causes a standing wave to be set up on the line with periodic maxima and minima collectively, extrema due to alternating constructive and destructive interference.

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Slot liner -

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