The magnetic force on a current-carrying wire in a magnetic field is calculated using the formula \(\vec{F} = I (\vec{L} \times \vec{B})\).
Given values are:
The cross product \(\vec{L} \times \vec{B}\) is computed as follows:
\(\vec{L} \times \vec{B} = (0.01 \, \hat{i}) \times [(0.4 \times 10^{-3} \hat{j}) + (0.6 \times 10^{-3} \hat{k})]\)
Utilizing the vector cross product rules:
\((\hat{i} \times \hat{j}) = \hat{k}\)
\((\hat{i} \times \hat{k}) = -\hat{j}\)
This results in:
\(\vec{L} \times \vec{B} = 0.01 \{(0.4 \times 10^{-3}) \hat{k} - (0.6 \times 10^{-3}) \hat{j}\}\)
\(\vec{L} \times \vec{B} = (0.4 \times 10^{-5} \hat{k} - 0.6 \times 10^{-5} \hat{j})\)
Now, the force \(\vec{F} = I (\vec{L} \times \vec{B})\) is calculated:
\(\vec{F} = 0.5 (0.4 \times 10^{-5} \hat{k} - 0.6 \times 10^{-5} \hat{j})\)
\(\vec{F} = (0.2 \times 10^{-5} \hat{k} - 0.3 \times 10^{-5} \hat{j})\)
This can be written as:
\(\vec{F} = (2 \hat{k} - 3 \hat{j}) \times 10^{-6} \text{N}\)
Expressing the force in micronewtons (\(\mu\text{N}\)):
\(\vec{F} = (-3 \hat{j} + 2 \hat{k}) \, \mu\text{N}\)
The resultant force acting on the wire segment is \( (-3 \hat{j} + 2 \hat{k}) \, \mu\text{N} \).