Work done moving charge near a line of charge

In summary, the problem involves finding the work required to move a charge of 2 microC from one point to another in a medium with relative permittivity of 3.7, near a line charge with a charge density of +329 microC/m. This can be done by calculating the potential due to the line charge and integrating it along the path from the initial point to the final point. The calculation can be simplified by breaking the line charge into small elements and adding/integrating their individual contributions. The expression for potential is V=(charge/length)ln(R)/(2pi(relative permittivity)), where R represents the distance from the point to the line charge. It is important to consider all points along the path, including
  • #1
Teameister
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Homework Statement


How much work (in J) is required to bring a charge of 2 microC from the point {2*6.8,-7,2*1.1}cm via the point {10,20,1}cm to the point {-3*6.8,3.4,-3*1.1}cm, in a medium with relative permittivity of 3.7, near a line charge along x=6.8 cm, z=1.1 cm, with charge density +329 microC/m? (Hint: what is the sign of the answer? Note that * simply means scalar multiplication)

Homework Equations


V= integral (E.dl) yields V=(charge/length)ln(R)/(2pi(relative permittivity)
W=Q(deltaV)

The Attempt at a Solution


I've tried to calculate the voltage at the first point but get a huge number assuming the line of point charges is acting as a cylindrical charge at the first point then same for middle point and last then using W=Q(deltaV).

No success.

Could someone please point me in the right direction.

Do I even need to consider the middle point?

Thank you.
 
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  • #2
Teameister said:
How much work (in J) is required to bring a charge of 2 microC from the point {2*6.8,-7,2*1.1}cm via the point {10,20,1}cm to the point {-3*6.8,3.4,-3*1.1}cm, in a medium with relative permittivity of 3.7, near a line charge along x=6.8 cm, z=1.1 cm, with charge density +329 microC/m? (Hint: what is the sign of the answer? Note that * simply means scalar multiplication)

Homework Equations


V= integral (E.dl) yields V=(charge/length)ln(R)/(2pi(relative permittivity)
W=Q(deltaV)

you have three points and a charge to be carried -the possible way is to calculate the potential due to line of charge(a finite distribution)
the way is to break the line distribution in 'small elements' and calculate the resultant field by adding and/ integrating along the full line so that all charges are accounted for and then proceed further.
i do not understand how you write the expression for potential and what is R?
 
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  • #3
Teameister said:
Could someone please point me in the right direction.
Please show your work instead of just describing it.
 

What is work done in moving charge near a line of charge?

The work done in moving charge near a line of charge refers to the amount of energy required to move a charged particle from one point to another in the vicinity of a line of charge. This work is dependent on the electric field and the distance traveled by the particle.

What is the formula for calculating work done in moving charge near a line of charge?

The formula for calculating work done in moving charge near a line of charge is W = qEd, where W is the work done, q is the charge of the particle, E is the electric field, and d is the distance traveled by the particle.

How is the direction of work done in moving charge near a line of charge determined?

The direction of work done in moving charge near a line of charge is determined by the direction of the electric field. If the electric field is in the same direction as the movement of the particle, then the work done is positive. If the electric field is in the opposite direction of the particle's movement, then the work done is negative.

What is the relationship between work done and potential difference in moving charge near a line of charge?

The relationship between work done and potential difference in moving charge near a line of charge is given by the equation W = q(Vb - Va), where W is the work done, q is the charge of the particle, and Vb and Va are the potential differences at the end points of the particle's movement. This shows that the work done is equal to the change in potential energy of the particle.

What are some real-life applications of work done in moving charge near a line of charge?

One real-life application of work done in moving charge near a line of charge is in the operation of particle accelerators, where charged particles are accelerated through electric fields to high speeds. Another application is in the charging of batteries, where work is done to move charged particles from one electrode to another. This concept is also important in understanding the behavior of lightning, where charge is moved through the atmosphere by electric fields.

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