Force acting on a charge across a hybrid medium

In summary, the force on charge ##q_2## due to the electric field in medium with dielectric ##K_2## is directly proportional to the charge and inversely proportional to the square of the distance between the two charges. When crossing the boundary between dielectrics, the electric field strength changes according to the dielectric constant of the new medium, but the electric field itself remains continuous.
  • #1
vcsharp2003
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Homework Statement
Two charge ##q_1## and ##q_2## are separated by two different dielectrics as shown in the diagram, having dielectric constants of ##K_1## and ##K_2##. The two charges are separated by a distance ##a##. What would be the force on charge ##q_2## due to charge ##q_1##?
Relevant Equations
##F = \dfrac {kq_1q_2} {Kr^2}##, where k is Coulomb's constant and K is dielectric constant, F is force of attraction between the two charges ##q_1## and ##q_2## that are separated by a distance ##r##

##E = \dfrac {kq} {Kr^2}##, where E is electric field due to a charge ##q## at a distance ##r## in medium having a dielectric constant ##K##
The force on charge ##q_2## will depend on the electric field in medium with dielectric ##K_2##.

Electric field in this second dielectric due to ##q_1## is ##E = \dfrac {kq_1} {K_2r^2}## where r would be the distance from ##q_1##.
So, the electric field at the point where charge ##q_2## is there would be ##E = \dfrac {kq_1} {K_2a^2}##

Therefore, force on second charge due to first charge would ##F_{21} = \dfrac {kq_1q_2} {K_2a^2} ##.
IMG_20211023_134338__01.jpg
 
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  • #2
Your answer would be correct if the entire distance ##a## had dielectric ##K_2##. The electric field at the boundary between dielectrics is ##\dfrac{kq_1}{K_1(\frac{3}{4}a)^2}##. What happens to it when you cross that boundary? In other words, what is continuous across the boundary?
 
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  • #3
kuruman said:
Your answer would be correct if the entire distance ##a## had dielectric ##K_2##. The electric field at the boundary between dielectrics is ##\dfrac{kq_1}{K_1(\frac{3}{4}a)^2}##. What happens to it when you cross that boundary? In other words, what is continuous across the boundary?
Thankyou for the answer.

My understanding is that the electric field in a medium becomes ##\dfrac {1} {K} ## times the electric field without any medium i.e. when there is vacuum, and I based my answer on this fact.

When the boundary of dielectrics is crossed from ##K_1## to ##K_2## then the electric field is still there except now it has a different formula i.e. a different strength, so electric field strength should not be a continuous function.
 
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FAQ: Force acting on a charge across a hybrid medium

What is the definition of force acting on a charge across a hybrid medium?

The force acting on a charge across a hybrid medium is the interaction between the charge and the medium, which can be a combination of different materials such as solids, liquids, and gases.

How is the force calculated in this scenario?

The force acting on a charge across a hybrid medium can be calculated using Coulomb's law, which states that the force is directly proportional to the product of the charges and inversely proportional to the square of the distance between them.

What factors can affect the force acting on a charge across a hybrid medium?

The force acting on a charge across a hybrid medium can be affected by the magnitude of the charges, the distance between them, and the dielectric constant of the medium.

Can the direction of the force change in a hybrid medium?

Yes, the direction of the force acting on a charge across a hybrid medium can change depending on the relative positions of the charges and the properties of the medium.

How does the force acting on a charge across a hybrid medium affect the motion of the charge?

The force acting on a charge across a hybrid medium can cause the charge to accelerate or decelerate depending on the direction of the force and the initial velocity of the charge. It can also change the direction of the charge's motion if the force is not acting in the same direction as the charge's velocity.

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