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If a uniform magnetic field is parallel to the plane of a surface, the magnetic flux through the surface is _______.
infinite
zero
maximum
half of maximum
maximum
The magnetic flux through a surface is defined as the number of magnetic field lines passing perpendicular to the area. If the magnetic field is parallel to the plane of the surface, the angle between the magnetic field vector and the area vector is 90┬░, resulting in zero magnetic flux.
The magnetic flux through a surface is defined as the number of magnetic field lines passing perpendicular to the area. If the magnetic field is parallel to the plane of the surface, the angle between the magnetic field vector and the area vector is 90┬░, resulting in zero magnetic flux.
Imagine holding a flat sheet of paper parallel to a steady stream of water (the magnetic field); none of the water passes through the surface of the paper.
Flux is flow: If the flow is parallel to the 'wall', it hits nothingтАФso Flux is zero.
╬жBтАЛ=BтЛЕA тАФ Definition of magnetic flux as a dot product
╬жBтАЛ=BAcos(╬╕) тАФ Scalar form involving the angle with the normal
The magnetic flux ╬жBтАЛ is calculated using the dot product ╬жBтАЛ=BтЛЕA=BAcos(╬╕), where ╬╕ is the angle between the magnetic field B and the normal vector A to the surface. When the field is parallel to the plane, it is perpendicular to the normal vector, meaning ╬╕=90┬░. Since cos(90┬░)=0, the magnetic flux is zero.
Magnetic flux is a scalar quantity.
The area vector A is always defined as normal (perpendicular) to the surface.
Maximum flux occurs when the field lines are perpendicular to the surface (╬╕=0┬░).
Design of electric generators
Understanding electromagnetic induction
The SI unit of magnetic flux is the Weber (Wb).
Option C is incorrect as labeled in the prompt; the correct answer is Option B because when ╬╕=90┬░, cos(90┬░)=0.
B is correct тАФ If the magnetic field is parallel to the surface, the angle between the field and the area normal is 90┬░, making the dot product cos(90┬░) equal to zero.
Always identify the direction of the area vector (the normal) first in flux problems to avoid common sign or ratio errors.