When a piece of aluminum wire of finite length is drawn through a series of dies to reduce its diameter to half its original value, its resistance will become :
1. Two times
2. Four times
3. Eight times
4. Sixteen times
Through a semiconductor, an electric current is due to drift off:
1. Free electrons
2. Free electrons and holes
3. Positive and negative ions
4. Protons
1. | proportional to \(T\). | 2. | proportional to\(\sqrt{T} \) |
3. | zero. | 4. | finite but independent of temperature. |
The specific resistance of all metals is most affected by :
1. Temperature
2. Pressure
3. Degree of illumination
4. Applied magnetic field
The positive temperature coefficient of resistance is for :
1. Carbon
2. Germanium
3. Copper
4. An electrolyte
The electric intensity E, current density j and specific resistance k are related to each other by the relation :
1. E = j/k
2. E = jk
3. E = k/j
4. k = jE
The resistance of a wire of uniform diameter d and length L is R. The resistance of another wire of the same material but diameter 2d and length 4L will be :
1. 2R
2. R
3. R/2
4. R/4
There is a current of 1.344 amp in a copper wire whose area of cross-section normal to the length of the wire is 1 mm2. If the number of free electrons per cm3 is 8.4 × 1022, then the drift velocity would be :
1. 1.0 mm/sec
2. 1.0 m/sec
3. 0.1 mm/sec
4. 0.01 mm/sec
An electric wire of length ‘I’ and area of cross-section a has a resistance R ohms. Another wire of the same material having the same length and area of cross-section 4a has a resistance of :
1. 4R
2. R/4
3. R/16
4. 16R
If \(n\), \(e\), \(\tau\) and \(m\) respectively represent the density, charge relaxation time and mass of the electron, then the resistance of a wire of length \(l\) and area of cross-section \(A\) will be:
1. \(\frac{ml}{ne^2\tau A}\)
2. \(\frac{m\tau^2A}{ne^2l}\)
3. \(\frac{ne^2\tau A}{2ml}\)
4. \(\frac{ne^2 A}{2m\tau l}\)