Chapter 4 b. Selectivity
Chapter 4b. Selectivity
Resonance
• Resonance in AC circuit is a special frequency
determined by the values of the: Resistance,
capacitance and inductance
• For series resonance the condition of resonance
is characterized by minimum impedance and
zero phase
• Parallel resonance, which is more common in
electronic practice, requires a more careful
definition
Series Resonance
• The resonance of a series RLC circuit occurs
when the inductive and capacitive reactance are
equal in magnitude but cancel each other
because the are 1800 degrees apart in phase
• The sharp minimum in impedance which occurs
is useful in tuning applications
• The sharpness of the minimum depends on the
values of R and is characterized by the “Q” of the
circuit.
Series RLC Circuit Variation reactance with frequency
Series Resonance
𝑋𝐿 = 𝑋𝐶
𝑋𝐿 = 2𝜋𝑓𝑟𝐿
𝑋𝐶 =1
2𝜋𝑓𝑟𝐶
2𝜋𝑓𝑟𝐿 =1
2𝜋𝑓𝑟𝐶
𝑓𝑟 =1
2𝜋 𝐿𝐶
𝐿 =1
4𝜋2𝑓2𝐶𝐶 =
1
4𝜋2𝑓2𝐿
Example: The capacitance that will resonate at a frequency of
18 MHz with a 12-μH inductor is determined as follows:
𝐶 =1
4𝜋2𝑓2𝐿=
1
39,478 18 × 106 2(12 × 10−6)
𝐶 =1
39,478 3,24 × 1014 2(12 × 10−6)= 6,5 × 10−12𝐹 𝑜𝑟 6,5 𝑝𝐹
Series Resonant
• Basic definition of resonance in a series tuned
circuit is the point at which XL equals XC
• With this condition, only the resistance of the
circuit impedes the current
• The total circuit impedance at resonance is Z = R
• Resonance in a series tuned circuit can also be
defined as th epoint at which the circuit
impedance is lowest and the circuit current is
highest
Series Resonant
• Since the circuit is resistive at resonance, the
current is in phase with the applied voltage
• Above the resonance frequency, the inductive
reactance is higher than the capacitive
reactance, and the inductor votage drop is
greater than the capacitor voltage drop
• Therefore the circuit is inductive, and the
current will lag the applied voltage
Series Resonant
• Below resonance, the capacitive reactance is
higher than the inductive reactance
• The net reactance is capacitive, producing a
leading current in the circuit
• The capacitor voltage drop is higher than the
inductor voltage drop
Series Resonant
Series Resonant
• Figure above is plot of frequency and phase shift
of the current in the circuit with respect to
frequency
• At very low frequencies, the capacitive reactance
is much greater than the inductive reactance,
therefore the current in the circuit is very low
because of the high impedance
Series Resonant
• If the circuit is predominantly capacitive, the
current leads the voltage by nearly 900
• As the frequency increases, XC goes down and XL
goes up
• The amount of leading phase shift decreases
• As the value of reactances approach one another,
the current begin to rise
Series Resonant
• When XL equals XC their effects cancel and the
impedance in the circuit is just that of the
resistance
• This produces a current peak, where the current
is in phase with the voltage (00)
Series Resonant
• As the frequency continues to rise, XL becomes
greater than XC
• The impedance of th ecircuit increases and the
current decreases
• The circuit will predominantly inductive, the
current lags the applied voltage
Series Resonant
• If the output voltage were being taken from across
the resistor in figure (a), the response curve and
phase angle of the voltage would correspond to
those in figure (b)
(a) (b)
Series Resonant
• The current is
highest in a region
centered on the
resonant frequency
• The narrow
frequency range
over which the
current is highest is
called the
bandwidth
• The current is highest in a region centered on the
resonant frequency
• The narrow frequency range over which the
current is highest is called the bandwidth
Series Resonant
• The upper and lower boundaries of the
bandwidth are defined by two cutoff frequencies
designated f1 and f2• These cutoff frequencies occur where the current
amplitude is 70.7 percent of the peak current
• In the figure, the peak current is 2 mA, and the
current at both the lower (f1) and upper (f2) cutoff
frequency is 0.707 of 2 mA, or 1.414 mA
Series Resonant
• Current levels at which the response is down
70.7 percent are called the half-power point
because the power at the cutoff frequencies is
one-half the power peak of the curve
𝑃 = 𝐼2𝑅 = 0.707 𝐼𝑝𝑒𝑎𝑘2𝑅 = 0.5 𝐼𝑝𝑒𝑎𝑘
2𝑅
Series Resonant
• The bandwidth BW of the tuned circuit is defined
as the difference between the upper and lower
cutoff frequencies:
𝐵𝑊 = 𝑓2 − 𝑓1
Series Resonant
• For example, assuming a resonant frequency of
75 kHz and upper and lower cutoff frequencies of
76.5 and 73.5 kHz, respectively, the bandwidth
is BW = 76.5 – 73.5 = 3 kHz
Selectivity and Q of a Circuit
• Resonant circuit are used to respond selectivity
to signal of a given frequency while
discriminating against signals of different
frequencies
• If the response of the circuit is more narrowly
peaked around the chosen frequency, we say
that the circuit has higher “selectivity”.
Selectivity and Q of a Circuit
• A “quality factor” Q, as described below, is a
measure of that selectivity, and we speak of a
circuit having a “high Q” if it is more narrowly
selective
• The selectivity of a circuit is dependent upon the
amount of resistance in the circuit
• The smaller the resistance, the higher the “Q” for
given values of L and C
Selectivity and Q of a Circuit
• The bandwidth of a resonant circuit is
determined by the Q of the circuit
• Recall the Q of an inductor is ration of the
inductive reactance to the circuit resistance,
which includes the resistance of the inductor
plus any additional series resistance:
𝑄 =𝑋𝐿
𝑋𝑇and 𝐵𝑊 =
𝑓𝑟
𝑄
Selectivity and Q of a Circuit
• If the Q of a circuit resonant at 18 MHz is 50,
then the bandwidth is BW = 18/50 = 0.36 MHz =
360 kHz
• The higher of resistance value, then lower the Q
value, the lower the Q, caused the higher of BW
Selectivity and Q of a Circuit
Selectivity and Q of a Circuit
• Question: What is the Q if Assuming a resonant
frequency of 75 kHz and upper and lower cutoff
frequencies of 76.5 and 73.5 kHz?
• Answer : 𝑄 =𝑓𝑟
𝐵𝑊=
75 𝑘𝐻𝑧
76.5 −73.5=
75 𝑘𝐻𝑧
3= 25
Selectivity and Q of a Circuit
• Since the bandwidth is approximately centered
on the resonant frequency, f1 is the sae distance
from fr as f2 is from fr• This fact allows you to calculate the resonant
frequency by knowing only the cutoff
frequencies:
𝑓𝑟 = 𝑓1 × 𝑓2
Selectivity and Q of a Circuit
• For example: if f1 = 175 kHz and f2 = 178 kHz,
the resonan frequency is
𝑓𝑟 = 175 × 103 × 178 × 103 = 176.5 𝑘𝐻𝑧
Selectivity and Q of a Circuit
• For a linear frequency scale, you can calculate
the center or resonant frequency by using an
average of the cutoff frequencies
𝑓𝑟 =𝑓1 + 𝑓22
Selectivity and Q of a Circuit
Selectivity and Q of a Circuit
Selectivity and Q of a Circuit
Selectivity and Q of a Circuit
Selectivity and Q of a Circuit