Acceleration of Bar in Circuit with Magnetic Field

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Homework Help Overview

The problem involves a metal bar in a magnetic field and its acceleration when a circuit is activated. The bar has a specified weight and resistance, and it is placed within a uniform magnetic field. Participants are exploring the dynamics of the system using Newton's laws and electromagnetic principles.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between the magnetic force, current, and the weight of the bar. There is confusion regarding the application of Newton's second law and the role of gravitational force in the context of horizontal motion.

Discussion Status

Some participants have offered insights into the assumptions regarding the weight of the bar and its implications for calculating mass. There is an ongoing exploration of why gravitational force is not considered in the net force equation for horizontal motion, with some clarification provided about the direction of forces involved.

Contextual Notes

Participants are working under the assumption that the bar's movement is restricted to the horizontal plane, which influences the application of forces in their calculations. The gravitational acceleration is assumed to be that of Earth for mass determination.

Mysterious
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Homework Statement


A 2.60-N metal bar, 1.50 m long and having a resistance of 10.0 Ω, rests horizontally on conducting wires connecting it to the circuit shown below. The bar is in a uniform, horizontal, 1.60-T magnetic field and is not attached to the wires in the circuit. What is the acceleration of the bar just after the switch S is closed?

OI9ZbAl.jpg


Homework Equations


Well, the magnetic force of a straight wire is valid here.
F = IlB‎sin‎Ø

And Newton's Second Law as well. Fnet = ma.
So combining the two equations, I get IlBsin‎Ø - mg = ma and thus a = (IlBsin‎Ø - mg)/m.

Also, since we have the potential difference of the source, ε = IR is valid as well.

The Attempt at a Solution


The equivalent of the parallel resistors in 5.0 Ω and the total (equivalent of the series) is 30.0 Ω.
From that,
ε = IR
I = ε/R
I = (120 V)/(30 Ω)
I = 4.0 A

And the path splits in two before it reaches the bar, so the current that will pass through the bar is 2.0 A.

However, the application of N2L is confusing me. We are not given either the mass of the bar or the acceleration; just the net force of the bar (2.60-N). How do I determine the mass to use in N2L and ultimately obtain the acceleration?

Thanks.
 
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Mysterious said:
However, the application of N2L is confusing me. We are not given either the mass of the bar or the acceleration; just the net force of the bar (2.60-N). How do I determine the mass to use in N2L and ultimately obtain the acceleration?
I'm going to assume the 2.60 N is the weight of the bar. Knowing the gravitational acceleration of whatever planet the circuit is on (surface of Earth is probably a safe bet) should give you the mass of the bar.
 
milesyoung said:
I'm going to assume the 2.60 N is the weight of the bar. Knowing the gravitational acceleration of whatever planet the circuit is on (surface of Earth is probably a safe bet) should give you the mass of the bar.

That makes sense. However, it doesn't explain why the solutions manual does not consider the weight force of the bar when applying's N2L:

They solve
a = IlB/m
where m = 2.60 N/9.80 m/s^2 as you said. But I don't understand why it is not a = (IlB - mg)/m.
 
It's implied that the bar is restricted to horizontal movement. Gravity has no horizontal component, so it doesn't contribute to the net force acting on the bar in the horizontal direction.
 
milesyoung said:
It's implied that the bar is restricted to horizontal movement. Gravity has no horizontal component, so it doesn't contribute to the net force acting on the bar in the horizontal direction.

That makes perfect sense. Thank you so much.
 
You're welcome. Consider also that in Newton's second law:
<br /> \mathbf{F} = m \mathbf{a} \quad (1)<br />
##\mathbf{F}## and ##\mathbf{a}## are vectors, but we can express (1) component-wise as:
<br /> \begin{align}<br /> F_x &amp;= m a_x \quad (2)\\<br /> F_y &amp;= m a_y \quad (3)<br /> \end{align}<br />
where x and y subscripts refer to horizontal and vertical components, respectively.

In your example, we know that ##a_y## is zero due to physical restrictions, so we're really only concerned with (2). I hope you can see why:
Mysterious said:
a = (IlB - mg)/m
mixes up (2) and (3).
 

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