CV2/2
2Q2/C
C2/V
CV
A. CV2/2
Conductor
Outer sheath
Insulation
Uniformly all over
Current leads voltage by 90�
Current leads voltage by 180�
Current lags voltage by 90�
Current lags voltage by 180�
0.3 S
3.33 S
0.33 S
30 S
Charge
Field intensity
Current
Voltage
Ceramic
Polyster
Electrolytic
Bakelite
The sum of individual charges
Equal to the charge of either capacitors
Equal to the product of the charges
The quotient of the charges
12 ms
4.8 s
83.3 s
12 s
Mass
Moisture content
Temperature
Thickness
The frequency range for maximum power transfer
The difference between the highest and lowest frequencies of the oscillator
The separation of the half-power points
The frequency at which XL= XC
Increases two times
Increases four times
Decreases two times
Decreases four times
2.592 x 105C
2.592 x 103 C
2.592 x 108 C
2.592 x 1012 C
Form factor
Peak factor
Dynamic factor
Leakage factor
It has reactance in radio-frequency circuits
It cannot handle much power
It draws a large amount of current
It cannot handle high voltage
Phase angle of the circuit is always 45�
Voltage across the inductance must be 90� out o f-phase witht he applied voltage
Current through the inductance lags its induced voltage by 90�
Current through the inductance and voltage across it are180� outof-phase
Resistor
Capacitor
Inductor
Both inductor and capacitor
Resistivity
Specific resistance
Coefficient of temperature change
Temperature coefficient of resistance
Decreases
Increases
Decreases or increases
Decreasesa increases or remains the same
Reluctance
Susceptance
Elastance
Conductance
Power absorbed is maximum
Power absorbed is minimum
Power absorbed is zero
The impedance is minimum
Length
Resistivity
Cross-sectional area
Mass
Smaller than the smallest capacitor
Smaller than the largest capacitor
Greater than any of the capacitor
Greater than the largest capacitor
10.1 kHz
10.1 MHz
101 MHz
101 kHz
Leading
Lagging
Zero
Unity
Resistivity
Cross-sectional area
Mass
Length
The greater the bandwidth
The narrower the passband
The broader the resonance curve
The wider the passband
Voltage across the inductance leads the voltage across the resistance by 90°
Resistive branch current is 90° out of phase with the inductive branch current
Resistive and inductive branch currents have the same phase
Resistive and inductive branch currents are 180° outof-phase
900 k
900 M
900 G
2/V
AV
A2
J/s