Magnetic Fields and Acceleration

AI Thread Summary
A particle with a mass of 1.81 x 10^-3 kg and a charge of 1.22 x 10^-8 C is moving in a magnetic field defined by the vector B = (1.63 T)î + (0.980 T)ĵ. The initial calculation for the force using F = q(v × B) was incorrect due to neglecting the sine term related to the angle between the velocity and magnetic field vectors. The discussion highlights the importance of considering both the components of the magnetic field and the velocity when calculating the cross product. The issue was resolved by recognizing the need to analyze the components of the magnetic field relative to the velocity. Properly applying these principles leads to the correct calculation of the particle's acceleration.
erik-the-red
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A particle with mass 1.81 \times 10^{-3}\;{\rm kg} and a charge of 1.22 \times 10^{-8}\;{\rm C} has, at a given instant, a velocity \vec{v} = (3.00 \times 10^{4}\;{\rm m}/{\rm s})\hat{j}.

What is the magnitude of the particle's acceleration produced by a uniform magnetic field \vec{B}=(1.63\;{\rm T})\hat{i} + (0.980\;{\rm T})\hat{j}?

I use the equation F = qv (CROSS) B.

I rewrite this as F = q*v*B*sin().

I plug into get F = (1.22*10^(-8))*(3.00*10^(4))*(1.90) and get (6.96*10^(-4)).

I divide this by the mass, but my answer is wrong.

Obviously my procedure is not correct. What's up?
 
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You forgot the sine term.
 
So the angle is not 90 degrees?
 
Most certainly not. You have two vectors, one with only j component, but the other has i and j components. You could just compute the cross product, or you could figure out the angle. Or you could break the problem into two components: B parallel to v and B perpendicular to v.
 
I just figured it out. Thanks!
 
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