Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN: 9780133923605
Author: Robert L. Boylestad
Publisher: PEARSON
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- Write the process and steps to design lead and leg compensator for steady state analysis of dynamic systems.arrow_forwardQ2] For the circuit shown below, when the switch closed at =0 and by assuming zero initial charge on the capacitor terminals. Do as required: a. Find the transient current equation wrt time. b. Identify the state of circuit. c. Find Neper frequency, resonant radian frequency, damping radian frequency, and natural radian frequency d. The value of "C" that makes the circuit as critically-damping. VR VL 1002 0.3H 200V 75µF Vcarrow_forwardRI Rz Vo %3D 2R.R.CG. REZ 1.+ Redrawthe circuit-equivalentwhenoperatingat-a-DC-voltage(0Hz).1 VerifyusingKCL-that-the circuit-operation will-be-that-of a-non-invertingamplifier. 2.→ Redrawthe circuit-equivalentat-veryhigh-frequencies.-VerifythatVoutisshorted.-(Hint.-Note- thereactance at-thenon-invertinginputat-extremelyhighfrequencies.--What-will-bethe- voltage at-that-node?-What-doesthis-meanfor-the voltage at-Rf2?)1 3.+ Let-C1=C2..-Calculate thevaluesofC1-and-C2-for-a-cut-offfrequency of500-Hz-if-R1-and-R2. are-33kohm-and-choosereasonablevaluesof Rf1 and-RF2•50-thatthe-gain-at-low-frequenciesis- 4-dB.--1 4.→ Simulate the circuit-on-Multisim-andrepeatsteps4-and5-of-Part-1-again.--Produce its-Bode Plot- using-the AC-Sweepfunction.-Identify-the type of responsecurve andtheroll-offrate. +,arrow_forward
- Consider the series RLC circuit, represented in the Figure below: Figure - Series RLC circuit. The mathematical model that relates the circuit current as a function of the applied voltage source is given by the following differential equation: In this way, determine: a) The differential equation in the frequency domain, considering the circuit initially de-energized, that is, with zero initial conditions. b) Determine the current in the frequency domain as a function of the applied voltage. Preferably do it in a typeable form, handwriting hinders understandingarrow_forward6. Consider the circuit depieted in the figure below, R V,eiut where we shall assume that the input voltage can be written as Vin(t) = Re{Voet} with complex-valued Vg, and likewise that the output voltage Vout(t) = Re{Vje*} with complex-valued Vị. With j = V-1, the complex impedances of resistors, ca- pacitors, and inductors in this case are respectively given by ZR = R, Zc = ZL = jwL. (a) Determine Vı/Vo as a function the angular frequency w given the parameters R and C. (b) Evaluate Vi/Vo in the limit w +0 and in the limit w + o0. Is the circuit above a low-pass filter, a high-pass filter, or something else? warrow_forwardWrite an expression for the complex impedance of a parallel combination of an inductor, L, and a capacitor, C, as a function of frequency. Find the frequency at which the magnitude of the impedance becomes infinite. What happens to the phase of the impedance at this frequency? What current will the parallel combination draw from an ideal sinusoidal voltage source at this frequency?arrow_forward
- Theoretically obtain the expression of the voltage across the capacitor from the Experiment when the circuit is stimulated with a 5 V direct current voltage source. Assume that initially the capacitor is fully unloaded (null initial conditions). Graph the waveform obtained.arrow_forward9. Use SPICE or a similar circuit analysis package to simulate a Cockcroft-Walton multiplier with two stages (i.e., a circuit like that in Figure 5.19, but only up through C3, C4, and D4). The input is a 120 VRMS 60 Hz sine wave. Use C = 0.01 F. What maximum load can be supplied without dropping the steady-state output potential by more than 10%?arrow_forwardWhat are two real-world consequences of having to amplify the input to a system so that the output reaches a desired steady-state value? Related to Electroncis & Circuitsarrow_forward
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