First, you will need to convert to the frequency domain.
ZR = R; Zc = 1/(jwc); ZL = jwL; w = 50Hz*2pi = 100pi
ZR = 25 ohm; Zc = -j80 ohms; v = 240*cos(100pi + 0)V
Second, combine the impedances, in series.
Zeq = ZR + Zc = 25-j80 ohms
Finally use Ohm's law to find the current. v = i*Z
i = 240 V / 25-j80 ohms = 2.9*e^(j73)A
2.9*e^(j1.28) has a magnitude of 2.9A and a phase of 73 degrees.
Now, you may need to convert back to the time domain.
i = 2.9cos(100pi + 73)A
Emitter bypass capacitor is a capacitor which provide low impedance to AC and high impedance to DC . AC is shunt then only DC appears on RC and volage gain increses.
in a dc frequency=0 impedance is xc=1/2*pi*f*c so impedance infinite
At resonance, the L and C impedance cancels out, so the current can be calculated based on the resistance and applied voltage. Imagine increasing frequency of the supply from 0 Hz to very high. At low frequency, the impedance of the inductor is ~0 (defined as Zl = w*L*j), and the impedance of the capacitor is very large (defined as Zc = 1 / (w*C*j)). As you increase the frequency, the impedance of the capacitor will decrease, as the impedance of the inductor increases. At some point (the resonant frequency), these two will be equal, with opposite signs. After crossing the resonant frequency, the inductor impedance will continue growing larger than the capacitor impedance until the total impedance approaches infinite.
You can. Give an example, and someone here will help.
Yes, capacitors can be, and often are, used in DC circuits. At steady state DC conditions, the capacitor has near infinite impedance. Its value is in its ability to resist changes in voltage, so it can serve as a transient filter. There is almost always a small ceramic capacitor connected between VCC and ground next to IC's in a digital circuit, for that exact purpose.
It is beacause of the capacitor's impedance which is 1/jwc where w=2*PI*f where f=frequency. If frequency = zero then the impedance =1/0 which equals infinate impedance and therefore an open.
A capacitor impedance is equivalent to 1/jwC, where j = i = imaginary number, w = frequency, and C = capacitance in Farads.
To calculate the admittance if you are given the impedance, you take the inverse of the impedance ( that is 1/z).
Emitter bypass capacitor is a capacitor which provide low impedance to AC and high impedance to DC . AC is shunt then only DC appears on RC and volage gain increses.
the impedance of the capacitor is given by Xc=1/jwC where w=2*pi*f and for DC source f=0 hence Xc=infinity ie, the capacitor will provide infinite impedance for DC, or its Open circuit
A capacitor totally blocks DC current (it's an open circuit to it). The higher the frequency, the less resistance (impedance) the capacitor has.
The impedance of a component (inductor or capacitor) will change with frequency - resistor impedances will not. Inductor impedance - j*w*L Capacitor impedance - 1/(j*w*C) L = inductance, C = capacitance, j = i = imaginary number, w = frequency in radians The actual inductance and capacitance does not change with frequency, only the impedance.
in a dc frequency=0 impedance is xc=1/2*pi*f*c so impedance infinite
That term to me is incorrect it should be capacitance impedance. Resistance is linear impedance. CAPACITANCE will follow a vector caused by the capacitor value.
At resonance, the L and C impedance cancels out, so the current can be calculated based on the resistance and applied voltage. Imagine increasing frequency of the supply from 0 Hz to very high. At low frequency, the impedance of the inductor is ~0 (defined as Zl = w*L*j), and the impedance of the capacitor is very large (defined as Zc = 1 / (w*C*j)). As you increase the frequency, the impedance of the capacitor will decrease, as the impedance of the inductor increases. At some point (the resonant frequency), these two will be equal, with opposite signs. After crossing the resonant frequency, the inductor impedance will continue growing larger than the capacitor impedance until the total impedance approaches infinite.
The tube or the FET transistor is used to build an impedance converter from the high impedance of the capacitor (condenser) of about 1 Giga ohms or more to the low impedance of the microphone output, which is less than 150 ohms.
You can. Give an example, and someone here will help.