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LT5571 - 620MHz – 1100MHz High Linearity Direct Quadrature Modulator.
LT5571 - 620MHz – 1100MHz High Linearity Direct Quadrature Modulator.

Lecture 7 Circuit analysis via Laplace transform
Lecture 7 Circuit analysis via Laplace transform

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Drake L7 Linear Amplifier Operator`s Manual

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... For this, you will have to build the circuit 3 times, once with each of R, L or C being connected to ground, such that Vout can be measured across this component. Does it matter in which order you place the other two components? [The ground lead of the oscilloscope probe must be connected to the cir ...
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... energy harvester is generally designed to be 50 Ohm [4]. Since the antenna can connect to the energy harvester directly, maximum power transfer between antenna and energy harvester can be achieved if the impedance is matched between the antenna and the energy harvester, while at the same time achiev ...
Playmaster No. 11 amplifier
Playmaster No. 11 amplifier

... EC2= 300V indicates an 8K P-P (2K line) is quite appropriate, and plate dissipation just extends dynamically into high levels, depending on initial bias level and VS2 sag. The maximum output valve bias current allowed is dependant on the maximum recommended plate dissipation of 12W for the EL84/6BQ5 ...
RF3166 QUAD-BAND GSM850/GSM900/DCS/PCS POWER AMP MODULE Features
RF3166 QUAD-BAND GSM850/GSM900/DCS/PCS POWER AMP MODULE Features

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Picoammeter/ Voltage Source

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A resistor is connected across an ac source as shown. For this circuit

... In the transformer shown in the drawing, there are more turns in the secondary than in the primary. In this situation, the voltage amplitude is A. greater in the primary than in the secondary. B. smaller in the primary than in the secondary. C. the same in the primary and in the secondary. D. not en ...
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Transmission at 200 Mbps in VME Card Cage

... floating line on either side of the signal pair. For comparison, data were also collected (not presented here) on a channel at the edge of the backplane. It was found that at the edge of the backplane, the crosstalk was reduced, as evidenced by improved BERT results and a more open eye pattern. To p ...
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Laboratory Manual for AC Electrical Circuits

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Laboratory Manual for AC Electrical Circuits

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Lab_module 3 - UniMAP Portal

... 2. Become aware of an experimental procedure to determine VTh, IN and RTh or RN. Hence the Thevenin and Norton equivalent circuits. 3. Demonstrate the conditions for maximum power transfer to a load are RL = RTh and VL = VTh/2. INTRODUCTION Through the use of Thevenin’s and Norton’s theorems, a comp ...
XR-2206 - TU Berlin
XR-2206 - TU Berlin

LT1969 - Dual 700MHz, 200mA, Adjustable Current Operational Amplifier
LT1969 - Dual 700MHz, 200mA, Adjustable Current Operational Amplifier

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Alternating Current Theory - JR Lucas
Alternating Current Theory - JR Lucas

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Standing wave ratio



In radio engineering and telecommunications, standing wave ratio (SWR) is a measure of impedance matching of loads to the characteristic impedance of a transmission line or waveguide. Impedance mismatches result in standing waves along the transmission line, and SWR is defined as the ratio of the partial standing wave's amplitude at an antinode (maximum) to the amplitude at a node (minimum) along the line.The SWR is usually thought of in terms of the maximum and minimum AC voltages along the transmission line, thus called the voltage standing wave ratio or VSWR (sometimes pronounced ""viswar""). For example, the VSWR value 1.2:1 denotes an AC voltage due to standing waves along the transmission line reaching a peak value 1.2 times that of the minimum AC voltage along that line. The SWR can as well be defined as the ratio of the maximum amplitude to minimum amplitude of the transmission line's currents, electric field strength, or the magnetic field strength. Neglecting transmission line loss, these ratios are identical.The power standing wave ratio (PSWR) is defined as the square of the VSWR, however this terminology has no physical relation to actual powers involved in transmission.The SWR can be measured with an instrument called an SWR meter. Since SWR is defined relative to the transmission line's characteristic impedance, the SWR meter must be constructed for that impedance; in practice most transmission lines used in these applications are coaxial cables with an impedance of either 50 or 75 ohms. Checking the SWR is a standard procedure in a radio station, for instance, to verify impedance matching of the antenna to the transmission line (and transmitter). Unlike connecting an impedance analyzer (or ""impedance bridge"") directly to the antenna (or other load), the SWR does not measure the actual impedance of the load, but quantifies the magnitude of the impedance mismatch just performing a measurement on the transmitter side of the transmission line.
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