Magnetic conductivity
Magnetic susceptibility
Electric conductivity
Electric susceptibility
A. Magnetic conductivity
Working voltage
Type of dielectric
Capacitance
All of the above
Square wave
Triangular wave
Trapezoidal wave
Sawtooth wave
Sinusoidal
Square wave
Triangular
Sawtooth
The greater the bandwidth
The narrower the passband
The broader the resonance curve
The wider the passband
XL= XC
XL= R
Z = R
Both A and C
Power factor
Reactive factor
Dissipation factor
1/Q factor
Less than the smallest resistance in the connection
Greater than the smallest resistance in the connection
Between the smallest and greatest resistance in the connection
Increasing and decreasing depending upon the supply voltage
1.65 kHz
16.5 MHz
16.5 kHz
165 kHz
Wire-wound resistor
Carbon-composition resistor
Potentiometer
Rheostat
Terminals
Plates
Dielectric
Air
Resistivity
Specific resistance
Coefficient of temperature change
Temperature coefficient of resistance
Impedance
Capacitive reactance
Resistance
Inductive reactance
Inductive
Conductive
Resistive
Capacitive
Infinite
RZ
XC/Z
XL/Z
R/Z
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
50 V
100 V
200 V
400 V
Peak
Average
Rms
Instantaneous
Wattage
Ohmic
Current
Voltage
Supplies energy
Receives energy
Both supplies and receives energy
Attenuates signal
190 ; 10 %
19 k ; 2 %
19 k ; 20 %
1.9 k ; 2 %
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
The current is zero in all the other resistances
The current is maximum in all the other resistances
The voltage is zero across the open resistance
The voltage is infinite across the open resistance
CV2
C2/J
C/V
J/V2
Passing a voltage proportional to the rate of change of current
Acting as a short circuit at time equal to zero
Passing a current proportional to the rate of change of voltage
Acting as a short circuit at time equal to infinity
Zero
1.3 k
Current lags voltage by less than 90�
Current lags voltage by 180�
Current lags voltage by 90�
Current leads voltage by 90�
Permittivity
Field intensity
Permeability
Elasticity