Calculating Work Required to Rotate a Dipole in an Electric Field

In summary, the work done by the electric forces acting on the charges is equal to the work done by an external agent that rotates the dipole at a constant angular speed.
  • #1
Calpalned
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6

Homework Statement


A dipole consists of charges +e and −e separated by 0.57 nm . It is in an electric field 2.6×104 N/C .
What is the work required to rotate the dipole from being oriented parallel to the field to being antiparallel to the field?

Homework Equations


PE = (dipole moment)(electric field) ## = 2.37 * 10^{-24}##
Work = ##W = PE(\cos{\theta_2}-\cos{\theta_1}) ## (From textbook)
Antiparallel = ##\theta_2 = 180 ##
Parallel = ##\theta_1 = 0 ##

The Attempt at a Solution


When I plugged the numbers for the equation for work I got ## = -4.7 * 10^{-24}## The correct answer is positive. I don't think I made any math mistakes but I can show my work if requested (plugging in numbers) if needed. Thank you very much.
 
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  • #2
Calpalned said:
Work = ##W = PE(\cos{\theta_2}-\cos{\theta_1}) ## (From textbook)

Is this the work done by the electric forces acting on the charges as the dipole rotates or is it the work done by an external agent that rotates the dipole at constant angular speed?
 
  • #3
TSny said:
Is this the work done by the electric forces acting on the charges as the dipole rotates or is it the work done by an external agent that rotates the dipole at constant angular speed?
jodido.png

I think it's done by the electric field
 
Last edited:
  • #4
From the textbook's derivation, you can see that they use the torque produced by the electric forces acting on the charges. So, the work they calculate is the work done by the electric forces. But your problem statement is apparently asking for the work required by an external agent, like yourself, to rotate the dipole. To hold the dipole at some angle, you would need to apply a torque that is equal but opposite to the torque due to the electric forces. If you rotate the dipole at a steady rate, your torque is still equal and opposite to the torque due to the electric forces.
 
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  • #5
TSny said:
From the textbook's derivation, you can see that they use the torque produced by the electric forces acting on the charges. So, the work they calculate is the work done by the electric forces. But your problem statement is apparently asking for the work required by an external agent, like yourself, to rotate the dipole. To hold the dipole at some angle, you would need to apply a torque that is equal but opposite to the torque due to the electric forces. If you rotate the dipole at a steady rate, your torque is still equal and opposite to the torque due to the electric forces.
Thank you so much. Now it makes sense!
 

Related to Calculating Work Required to Rotate a Dipole in an Electric Field

What is Work Dipole Rotation (21.62)?

Work Dipole Rotation (21.62) refers to the physical phenomenon of a dipole (a pair of equal and opposite charges) experiencing a rotational force when placed in an external electric field. This is measured in joules and is described by the formula W = qEcosθ, where q is the magnitude of the charge, E is the strength of the electric field, and θ is the angle between the dipole and the direction of the field.

How is Work Dipole Rotation (21.62) calculated?

The amount of work done on a dipole due to rotation in an electric field can be calculated using the formula W = qEcosθ, where q is the magnitude of the charge, E is the strength of the electric field, and θ is the angle between the dipole and the direction of the field. This calculation is typically done in joules.

What is the significance of Work Dipole Rotation (21.62) in physics?

Work Dipole Rotation (21.62) is significant in physics because it helps us understand the behavior of dipoles in electric fields. This phenomenon is important in various fields of study such as electromagnetism, quantum mechanics, and molecular biology. It also has practical applications in technologies such as electric motors, generators, and sensors.

How does Work Dipole Rotation (21.62) differ from Work Electric Dipole?

Work Dipole Rotation (21.62) and Work Electric Dipole are two related but distinct concepts. Work Dipole Rotation (21.62) refers to the rotational force experienced by a dipole in an external electric field, while Work Electric Dipole refers to the work done on a dipole as it moves from one point to another in an electric field. Additionally, Work Electric Dipole is described by the formula W = -pEcosθ, where p is the dipole moment and E is the electric field.

Can Work Dipole Rotation (21.62) be negative?

Yes, Work Dipole Rotation (21.62) can be negative. The sign of the work done on a dipole by an electric field depends on the orientation of the dipole with respect to the field. If the dipole is perpendicular to the field, the work done will be zero. If the dipole is parallel to the field, the work done will be positive. If the dipole is anti-parallel to the field, the work done will be negative.

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