Input current = 15 × 10–6 Output current = 3 × 10–3 Resistance out put = 1000 Vinput = 10 × 10–3 Now Vinput = rinput × iinput 10 × 10–3 = rinput × 15 × 10–6 rinput =
Voltage gain =
Input current = 15 × 10–6 Output current = 3 × 10–3 Resistance out put = 1000 Vinput = 10 × 10–3 Now Vinput = rinput × iinput 10 × 10–3 = rinput × 15 × 10–6 rinput =
Voltage gain =
1.5 – 0.5 – R 10–2 = 0 R = 100
=
=
eV = 3.1 eV
(1) Multimeter shows deflection when it connects with capacitor.
(2) If we assume that LED has negligible resistance then multimeter shows no deflection for the forward bias but when it connects in reverse direction, it break down occurs so splash of light out.
(3) The resistance of metal wire may be taken zero, so no deflection in multimeter.
(4) No matter, how we connect the resistance across multimeter.
It shows same deflection.
In photodiode, photocurrent increases with increasing biasing voltage and then becomes saturated.
Given, emitter current, IE = 4 mA Collector current, IC = 3.5 mA Current gain in common base amplifier,
Also, current gain in common emitter amplifier,
S-1 : Statement 1 is false because in case of two discrete back to back connected diodes, there are four doped regions instead of three and there is nothing that resembles a thin base region between an emitter and a collector.
S-2 : Statement-2 is true, as we know that, amplification factor () is the ratio of collector current to base current.
The zener breakdown occurs in the heavily doped p-n junction diode.
Heavily doped p-n junction diodes have narrow depletion region.
In n-type semiconductor pentavalent impurity is added.
Each pentavalent impurity donates a free electron.
So the Fermi-level of n-type semiconductor will go upward.
And In p-type semiconductor trivalent impurity is added.
Each trivalent impurity creates a hole in the valence band.
So the Fermi-level of p-type semiconductor will go downward.
We know that
= 652.63 nm 654 nm Wavelength of red light is 620 nm to 750 nm