Acceleration of Bar in Circuit with Magnetic Field

In summary, a metal bar with a weight of 2.60 N and a resistance of 10.0 Ω is placed horizontally in a uniform magnetic field of 1.60 T, connected to a circuit with a potential difference of 120 V. After the switch S is closed, the bar experiences a net force of 2.60 N and a current of 2.0 A. Using Newton's second law and knowledge of the gravitational acceleration, the acceleration of the bar can be calculated as a = IlB/m. However, since the bar is restricted to horizontal movement, the weight force does not need to be considered in this calculation.
  • #1
Mysterious
5
0

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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  • #2
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.
 
  • #3
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.
 
  • #4
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.
 
  • #5
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.
 
  • #6
You're welcome. Consider also that in Newton's second law:
[tex]
\mathbf{F} = m \mathbf{a} \quad (1)
[/tex]
##\mathbf{F}## and ##\mathbf{a}## are vectors, but we can express (1) component-wise as:
[tex]
\begin{align}
F_x &= m a_x \quad (2)\\
F_y &= m a_y \quad (3)
\end{align}
[/tex]
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).
 

FAQ: Acceleration of Bar in Circuit with Magnetic Field

1. What is the concept behind "Acceleration of Bar in Circuit with Magnetic Field"?

The concept behind "Acceleration of Bar in Circuit with Magnetic Field" is based on the interaction between magnetic fields and electric currents. When an electric current flows through a wire, it creates a magnetic field around the wire. This magnetic field can then interact with another magnetic field, such as the one created by a permanent magnet, causing a force on the wire.

2. How does a magnetic field affect the acceleration of a bar in a circuit?

A magnetic field can cause a force on a bar in a circuit, which can then accelerate the bar. This is because the magnetic field interacts with the electric current in the wire, creating a force that pushes the bar in a specific direction. The strength and direction of the magnetic field, as well as the direction and magnitude of the electric current, will determine the acceleration of the bar.

3. What factors affect the acceleration of a bar in a circuit with a magnetic field?

The acceleration of a bar in a circuit with a magnetic field is affected by several factors, including the strength and direction of the magnetic field, the direction and magnitude of the electric current, the length and shape of the bar, and the material of the bar. Additionally, any external forces acting on the bar, such as friction, can also affect its acceleration.

4. How can the acceleration of a bar in a circuit with a magnetic field be calculated?

The acceleration of a bar in a circuit with a magnetic field can be calculated using the equation F = ma, where F is the force acting on the bar, m is the mass of the bar, and a is the acceleration. The force can be calculated using the formula F = I x L x B, where I is the electric current, L is the length of the bar, and B is the strength of the magnetic field. By combining these two equations, the acceleration of the bar can be determined.

5. What are the practical applications of studying the acceleration of a bar in a circuit with a magnetic field?

The study of the acceleration of a bar in a circuit with a magnetic field has many practical applications, including the development of electric motors and generators, as well as the design of magnetic levitation trains. It also helps us understand the principles behind electromagnetism and how it can be harnessed for various technological advancements.

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