Force acting on a charge across a hybrid medium

AI Thread Summary
The force acting on charge q2 is influenced by the electric field in the dielectric medium K2, calculated as E = kq1/(K2a^2). The force between charges q1 and q2 is given by F21 = kq1q2/(K2a^2), assuming the entire distance a is within dielectric K2. At the boundary between different dielectrics, the electric field changes and is expressed as kq1/(K1(3/4a)^2). The electric field strength is not continuous across the boundary, as it varies with the dielectric constants K1 and K2. Understanding these principles is crucial for analyzing forces in hybrid dielectric media.
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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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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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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