To find the mobility of the charge carrier, we start by using the formula for electric current: \(I = nAqv_d\), where:
- \(I\) is the current (1.2 A)
- \(n\) is the charge density (\(7.5 \times 10^{28} \, \text{m}^{-3}\))
- \(A\) is the cross-sectional area (\(0.2 \, \text{mm}^2 = 0.2 \times 10^{-6} \, \text{m}^2\))
- \(q\) is the charge of an electron (\(1.6 \times 10^{-19} \, \text{C}\))
- \(v_d\) is the drift velocity
Rearranging gives the drift velocity: \[v_d = \frac{I}{nAq} = \frac{1.2}{(7.5 \times 10^{28})(0.2 \times 10^{-6})(1.6 \times 10^{-19})}\]Calculating: \[v_d \approx 5 \times 10^{-5} \, \text{m/s}\]The mobility \(\mu\) is related to the drift velocity and electric field \(E\) by \(\mu = \frac{v_d}{E}\). The electric field \(E\) is calculated as: \[E = \frac{\text{Potential Difference}}{\text{Length}} = \frac{2}{2} = 1 \, \text{V/m}\]Thus, \(\mu = \frac{5 \times 10^{-5}}{1} = 5 \times 10^{-5} \, \text{m}^2/\text{V}\cdot\text{s} = 5 \times 10^{-4} \, \text{SI units}\) Therefore, \(x = 5\). This value, \(x = 5\), lies within the specified range of (5,5).