A straight wire carrying a current experiences a force when placed in a magnetic field due to the Lorentz force. The magnitude of this force can be calculated using the formula:
\( F = I \cdot L \cdot B \cdot \sin(\theta) \)
Where:
\( F \) = force on the wire (in Newtons)
\( I \) = current flowing through the wire (in Amperes)
\( L \) = length of the wire (in meters)
\( B \) = magnetic field strength (in Tesla)
\( \theta \) = angle between the wire and magnetic field (in degrees)
The given values are:
- \( I = 10 \, \text{A} \)
- \( L = 2 \, \text{m} \)
- \( B = 0.15 \, \text{T} \)
- \( \theta = 45^\circ \)
Plug these values into the formula:
\( F = 10 \cdot 2 \cdot 0.15 \cdot \sin(45^\circ) \)
Knowing that \(\sin(45^\circ) = \frac{\sqrt{2}}{2}\), we find:
\( F = 10 \cdot 2 \cdot 0.15 \cdot \frac{\sqrt{2}}{2} \)
This simplifies to:
\( F = 3 \cdot \sqrt{2} \cdot \frac{1}{2} \)
\( F = \frac{3\sqrt{2}}{2} \)
Therefore, the force on the wire is:
\( \frac{3}{\sqrt{2}} \, \text{N} \)