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Figure 4.1:
|
Electrical Circuits are the most common technological application
where we see resonances. The LCR circuit shown in Figure
4.1 characterizes the typical situation. The circuits
includes a signal generator which produces an AC signal of voltage
amplitude at frequency .
Applying Kirchoff's Law to this circuit we have,
|
which may be written solely in terms of the charge as
|
(4.2) |
We see that this is a damped oscillator with an external
sinusoidal force. The equation governing this is
|
(4.3) |
where
, and .
We next consider the power dissipated in this circuit. The resistance
is the only circuit element which draws power. We proceed to calculate
this by calculating the impedence
|
(4.4) |
which varies with frequency. The voltage and current are related as
, which gives the current
|
(4.5) |
The average power dissipated may be calculated as
which is
|
(4.6) |
Problem For an Electrical Oscillator with and
,
- a.
- what is the natural (angular) frequency ? ()
- b.
- Choose so that the oscillator is critically
damped. ()
- c.
- For
, what is the maximum power that can be
drawn from a source? ()
- d.
- What is the FWHM of the peak? ()
- e.
- At what frequency is half the maximum power drawn? ( and )
- f.
- What is the value of the quality factor ? (
)
- g.
- What is the time period of the oscillator? (
where
and
.)
- h.
- What is the value of the log decrement ?
(
,
)
Next: The Raman Effect
Up: Resonance.
Previous: Resonance.
Contents
Physics 1st Year
2009-01-06