Quick question on direction of dl in motional emf integral

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SUMMARY

The discussion centers on the direction of the differential length element (dl) in the context of the motional electromotive force (emf) integral, represented by the equation ∫ (u x B) ⋅ dl. It is established that the direction of dl is determined by the path taken from point a to point b, with positive direction towards point b. The cross product u x B is typically perpendicular to the velocity vector u, indicating that magnetic fields alter the direction of velocities without affecting their magnitude.

PREREQUISITES
  • Understanding of vector calculus, specifically line integrals.
  • Familiarity with electromagnetism concepts, particularly motional emf.
  • Knowledge of cross products and their geometric implications.
  • Basic comprehension of magnetic flux density (B) and its effects on charged particles.
NEXT STEPS
  • Study the principles of line integrals in vector calculus.
  • Learn about the applications of motional emf in real-world scenarios.
  • Explore the geometric interpretation of cross products in physics.
  • Investigate the effects of magnetic fields on charged particle motion.
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Students and professionals in physics, particularly those studying electromagnetism, as well as educators looking for clarification on the motional emf integral and its applications.

edsoneicc
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Homework Statement


u = velocity
B = magnetic flux density

Homework Equations


∫ (uxB)⋅dl

The Attempt at a Solution


From my understanding, the direction of dl depends on the resulting direction of (uxB). How will I know if my dl is in positive or negative?
 
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Hi Ed,

Little response so far eh? Perhaps because there is no problem statement ? And your equation isn't an equation ?
Attempts at solution usually look different also.

On the constructive side: in something like$$
X =\int_a^b (...) \cdot \vec {dl}$$ the direction of ##l## is established by the path to be followed from ##\vec a## to ##\vec b## : positive is towards ##\vec b##.

Since ##\vec u \times \vec B## is generally perpendicular to ##\vec u##, and ##\vec u## is generally along ##\vec {dl}##, the dot product is generally zero: magnetic fields have a tendency to change the direction of velocities but not the magnitude.
 

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