A wire is oriented along the x-axis. It is connected to two batteries, and a conventional current of 2.4 A runs through the wire, in the +x direction. Along 0.27 m of the length of the wire there is a magnetic field of 0.62 tesla in the +y direction, due to a large magnet nearby. At other locations in the circuit, the magnetic field due to external sources is negligible. What is the magnitude of the magnetic force on the wire?

Respuesta :

Answer:

[tex] \vec{F}=0.40176 N \hat{k} [/tex]

Explanation:

To calculate the force we need to use this equation

[tex]\vec{F}=\int\limits^L_0 {i(\vec{dl}\times\vec{B})}[/tex]

where L is the total length of the wire

So in this case the small element of current is

[tex] \vec{dl} = dx \hat{i} [/tex]

Because x is the direction of the current flow.

As is said in the problem B is such that

[tex] \vec{B} = B \hat{j} = 0.62\hat{j} [ T][/tex]

so to use the equation above we first calculate the following cross product:

[tex]\vec{dl}\times\vec{B}=dx \hat{i}\times B \hat{j} = Bdx\hat{k}[/tex]

so the force:

[tex] F = \int\limits^L_0 {i(\vec{dl}\times\vec{B})}=\int\limits^L_0{iBdx\hat{k}} [/tex]

So here we use the fact that B=0 in any point of the x axis that is not [tex] x^{'}=0.27 [m] [/tex], that means that we only need to do the integration between a very short distant behind the point [tex] x^{'}=0.27 [m] [/tex] and a very short distant after that point, meaning:

[tex]\vec{F}= \lim_{h \to 0}{\int\limits^{x^{'}+h}_{x^{'}-h}{iBdx\hat{k}} }[/tex]

so is the same as evaluating [tex]iBx[/tex] at [tex]x=x^{'}[/tex]

that is:

[tex] 2,4 A * 0,62 T * 0,27 m \hat{k}[/tex]

[tex] 2,4 A * 0,62 (\frac{Kg}{A s^{2}}) * 0,27 m \hat{k}[/tex]

[tex] 2,4*0,62*2,7 ( \frac{ kgm }{ s^{2} } ) \hat{k}[/tex]

[tex] \vec{F}=0.40176 N \hat{k} [/tex]

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