The ratio of dopant atoms to silicon atoms is given as: \[ \frac{\text{Number of dopant atoms}}{\text{Number of silicon atoms}} = \frac{1}{5 \times 10^7} \]
The number density of silicon atoms is \( 5 \times 10^{28} \) atoms/m\(^3\). The number of dopant atoms per cubic metre is: \[ \text{Number of dopant atoms} = \frac{1}{5 \times 10^7} \times 5 \times 10^{28} = 10^{21} \, \text{dopant atoms/m}^3 \]
Since each dopant atom creates one hole in the semiconductor, the number of holes created per cubic metre is equal to the number of dopant atoms: \[ \text{Number of holes} = 10^{21} \, \text{holes/m}^3 \]
Since \( 1 \, \text{m}^3 = 10^6 \, \text{cm}^3 \), the number of holes per cubic centimetre is: \[ \text{Number of holes} = \frac{10^{21}}{10^6} = 10^{15} \, \text{holes/cm}^3 \]
One example of a dopant used in p-type silicon is **boron (B)**. Boron atoms have one fewer valence electron than silicon, creating a hole in the crystal lattice when substituted for a silicon atom.
The number of holes created per cubic centimetre in the specimen due to doping is \( \boxed{10^{15}} \, \text{holes/cm}^3 \).
A short bar magnet placed with its axis at 30º with a uniform external magnetic field of 0.25 T experiences a torque of magnitude equal to 4.5 × 10-2 J. What is the magnitude of magnetic moment of the magnet?
A short bar magnet of magnetic moment m = 0.32 J T-1 is placed in a uniform magnetic field of 0.15 T. If the bar is free to rotate in the plane of the field, which orientation would correspond to its ( a ) stable, and ( b) unstable equilibrium? What is the potential energy of the magnet in each case?
A closely wound solenoid of 800 turns and area of cross section 2.5 × 10-4 m2 carries a current of 3.0 A. Explain the sense in which the solenoid acts like a bar magnet. What is its associated magnetic moment?