In a bipolar junction transistor (BJT):
$I_E$ (emitter current) is the total current leaving the emitter.
$I_C$ (collector current) and $I_B$ (base current) are components of $I_E$
According to Kirchhoff's Current Law (KCL): $I_E = I_C + I_B$.
Typically, $I_B$ is much smaller than $I_C$, making $I_E$ approximately equal to $I_C$.
| List-I | List-II |
| (A) XeF2 | (iii) Linear |
| (B) BF3 | (i) Trigonal Planar |
| (C) XeF4 | (ii) Distorted Octahedral |
| (D) SF6 | (iv) Regular Octahedral |
| List-I | List-II |
|---|---|
| (A) Linus Pauling | (iii) Electronegativity |
| (B) Albert Einstein | (ii) Photoelectric effect |
| (C) Ernest Rutherford | (i) Alpha particle scattering experiment |
| (D) Max Planck | (iv) Black body radiations |
| List-I | List-II |
|---|---|
| (A) Lyman | (i) n = 2, 3, 4, ... |
| (B) Balmer | (ii) n = 3, 4, 5, ... |
| (C) Paschen | (iii) n = 4, 5, 6, ... |
| (D) Bracket | (iv) n = 5, 6, 7, ... |