Chapter 23 Alternating Current Circuits
Chapter 23 Alternating Current Circuits. 23.1 Capacitors and Capacitive Reactance The resistance in a purely resistive circuit has the same value at all.
Dec 26, 2015
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Chapter 23
Alternating Current Circuits
23.1 Capacitors and Capacitive Reactance
The resistance in a purely resistive circuit has the same valueat all frequencies.
RIV rmsrms
23.1 Capacitors and Capacitive Reactance
CXIV rmsrms fC
XC 2
1
capacitive reactance
23.1 Capacitors and Capacitive Reactance
Example 1 A Capacitor in an AC Circuit
The capacitance is 1.50μF and the rms voltage is 25.0 V. What is the rms currentwhen the frequency is (a) 100 Hz and(b) 5000 Hz?
23.1 Capacitors and Capacitive Reactance
A 0236.01060
V 0.25rmsrms
CX
VI
1060F1050.1Hz 1002
1
2
16 fC
XC(a)
(b)
2.21F1050.1Hz 50002
1
2
16 fC
XC
A 18.121.2
V 0.25rmsrms
CX
VI
23.1 Capacitors and Capacitive Reactance
For a purely resistive circuit,the current and voltage arein phase.
23.1 Capacitors and Capacitive Reactance
The current in a capacitor leadsthe voltage across the capacitorby a phase angle of 90 degrees.
The average power used by a capacitor in an ac circuit is zero.
23.1 Capacitors and Capacitive Reactance
In the phasor model, the voltageand current are represented by rotating arrows (called phasors).
These phasors rotate at a frequency f.
The vertical component of the phasoris the instantaneous value of the currentor voltage.
23.2 Inductors and Inductive Reactance
LXIV rmsrms
inductive reactance
LfX L 2
23.2 Inductors and Inductive Reactance
The current lags behind the voltage by a phase angle of90 degrees.
The average power used by an inductor in an ac circuit is zero.
23.2 Inductors and Inductive Reactance
23.3 Circuits Containing Resistance, Capacitance, and Inductance
In a series RLC circuit, the total opposition to the flow is called the impedance.
ZIV rmsrms 22CL XXRZ
23.3 Circuits Containing Resistance, Capacitance, and Inductance
22CL XXRZ
23.3 Circuits Containing Resistance, Capacitance, and Inductance
R
XX
V
VV CL
R
CL
tan
phase angle between current and total voltage
coscos rmsrms2rms VIZIP
23.4 Resonance in Electric Circuits
Resonance occurs when the frequency of a vibrating force exactlymatches a natural (resonant) frequency of the object to which the force is applied.
The oscillation of a mass on a spring is analogous to the oscillation of the electric and magnetic fields that occur, respectively, in a capacitorand an inductor.
23.4 Resonance in Electric Circuits
22
rmsrms
212 fCfLR
VI
22 212 fCfLRZ
Resonant frequencyLC
fo 2
1
23.5 Semiconductor Devices
Semiconductor devices such as diodes and transistors are widelyused in modern electronics.
23.5 Semiconductor Devices
n-TYPE AND p-TYPE SEMICONDUCTORS
The semiconducting materials (silicon and germanium) used to make diodes and transistors are doped by adding smallamounts of an impurity element.
23.5 Semiconductor Devices
THE SEMICONDUCTOR DIODE
23.5 Semiconductor Devices
At the junction between the n and p materials, mobile electrons andholes combine and create positive and negative charge layers.
23.5 Semiconductor Devices
There is an appreciable current through the diode when the diode is forward biased.
Under a reverse bias, there is almost no current through the diode.
23.5 Semiconductor Devices
23.5 Semiconductor Devices
A half-wave rectifier.
23.5 Semiconductor Devices
SOLAR CELLS
23.5 Semiconductor Devices
TRANSISTORS
A bipolar junction transistor canbe used to amplify a smaller voltage into a larger one.
23.5 Semiconductor Devices
23.5 Semiconductor Devices
Related Documents
