The force on a current-carrying wire segment in a magnetic field is calculated using the formula:
\( \mathbf{F} = I \mathbf{L} \times \mathbf{B} \)
Where:
\( I = 0.5 \, \text{A} \) is the current, \( \mathbf{L} \) is the wire's length vector, and \( \mathbf{B} \) is the magnetic field vector.
The wire is 1 cm long and oriented along the x-axis, so \( \mathbf{L} = (0.01 \, \text{m}) \hat{i} \).
The magnetic field is given by:
\( \mathbf{B} = (0.4 \, \text{mT}) \hat{j} + (0.6 \, \text{mT}) \hat{k} \).
Converting to teslas:
\( \mathbf{B} = (0.4 \times 10^{-3} \, \text{T}) \hat{j} + (0.6 \times 10^{-3} \, \text{T}) \hat{k} \).
The cross product \( \mathbf{L} \times \mathbf{B} \) is calculated as:
\( \mathbf{L} \times \mathbf{B} = (0.01 \hat{i}) \times (0.4 \times 10^{-3} \hat{j} + 0.6 \times 10^{-3} \hat{k}) \)
Using cross product identities:
The result of the cross product is:
\( \mathbf{L} \times \mathbf{B} = 0.01(0.4 \times 10^{-3}) \hat{k} + 0.01(-0.6 \times 10^{-3}) (-\hat{j}) \)
\( = (0.4 \times 10^{-5}) \hat{k} - (0.6 \times 10^{-5}) \hat{j} \)
\( = (-0.6 \times 10^{-5}) \hat{j} + (0.4 \times 10^{-5}) \hat{k} \)
Multiplying by the current \( I = 0.5 \, \text{A} \):
\( \mathbf{F} = 0.5((-0.6 \times 10^{-5}) \hat{j} + (0.4 \times 10^{-5}) \hat{k}) \)
\( = (-0.3 \times 10^{-5} \, \text{N}) \hat{j} + (0.2 \times 10^{-5} \, \text{N}) \hat{k} \).
Converting to micronewtons (\( 1 \, \text{N} = 10^6 \, \mu\text{N} \)):
\( = (-3 \hat{j} + 2 \hat{k}) \, \mu\text{N} \).
The force on the wire segment is: \((-3\hat{j} + 2\hat{k}) \, \mu\text{N}\).
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by \(15\) cm length of wire \(Q\) is ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 