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source impedance वाक्य

"source impedance" हिंदी मेंsource impedance in a sentence
उदाहरण वाक्यमोबाइल
  • The generalized source impedance for a reactive ( inductive or capacitive ) source device is more complicated to determine, and is usually measured with specialized instruments, rather than taking many measurements by hand.
  • An alternative to impedance matching is impedance bridging, in which the load impedance is chosen to be much larger than the source impedance and maximizing voltage transfer, rather than power, is the goal.
  • At 200 MHz, a noise figure of 2.5 ( or 4 dB ) can be reached with the ECC2000 tube in an optimized " cascode "-circuit with an optimized source impedance.
  • If an even multiple is desired then an anti-parallel pair of diodes will suppress the odd local oscillator contribution, to the level that the diodes can be made identical and experience the same source impedance.
  • The Reamp inductively couples balanced line-level sources into unbalanced guitar-level destinations ( e . g ., DAW output to guitar amp input ) and includes a potentiometer which alters both signal level and source impedance.
  • If the source impedance remains constant and the fault current changes appreciably as we move away from the relay then it is advantageous to use IDMT overcurrent protection to achieve high speed protection over a large section of the protected circuit.
  • For larger source impedances, the gain is determined by the resistor ratio " R L / R S ", and not by the transistor properties, which can be an advantage where insensitivity to temperature or transistor variations is important.
  • Because no ideal sources of either variety exist ( all real-world examples have finite and non-zero source impedance ), any current source can be considered as a voltage source with the " same " source impedance and vice versa.
  • Because no ideal sources of either variety exist ( all real-world examples have finite and non-zero source impedance ), any current source can be considered as a voltage source with the " same " source impedance and vice versa.
  • Since no ideal sources of either variety exist ( all real-world examples have finite and non-zero source impedance ), any current source can be considered as a voltage source with the " same " source impedance and vice versa.
  • Since no ideal sources of either variety exist ( all real-world examples have finite and non-zero source impedance ), any current source can be considered as a voltage source with the " same " source impedance and vice versa.
  • In radio frequency transmission lines, and other electronics, there is often a requirement to match the source impedance ( at the transmitter ) to the load impedance ( such as an antenna ) to avoid reflections in the transmission line that could negatively impact the transmitter.
  • For amplifiers, this source impedance Z _ \ mathrm { source } ( also : output impedance ) is generally smaller than 0.1 ohm ( ? ), and from the point of view of the driver voice coil, is a near short-circuit.
  • P source, max may only be obtained from the source when the load impedance connected to it ( i . e . the equivalent input impedance of the two-port network ) is the complex conjugate of the source impedance, a consequence of the maximum power theorem.
  • This change would be due to the source impedance ( in this DC case, the source resistance ) of the battery, power supply, or generator plus the resistance of the power system and conductors connecting it to the motor, assuming that there is no voltage regulation at work to increase and decrease the supply voltage.
  • In this diagram, AC power is being transferred from the source, with phasor magnitude voltage | V _ \ mathrm { S } | ( peak voltage ) and fixed source impedance Z _ \ mathrm { S }, to a load with impedance Z _ \ mathrm { L }, resulting in a phasor magnitude current | I | . | I | is simply the source voltage divided by the total circuit impedance:
  • For instance, if there is a perfect match between the load impedance " Z " load and the source impedance " Z " source = " Z " * load, that perfect match will remain if the source and load are connected through a transmission line with an electrical length of one half wavelength ( or a multiple of one half wavelengths ) using a transmission line of " any " characteristic impedance " Z " 0.
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