Force acting on a charge across a hybrid medium

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SUMMARY

The force acting on charge q2 in a hybrid medium is determined by the electric field in the dielectric K2. The electric field due to charge q1 is expressed as E = kq1 / (K2r2), with the force on q2 calculated as F21 = kq1q2 / (K2a2). The electric field at the boundary between dielectrics K1 and K2 is kq1 / (K1(3/4a)2), indicating a change in electric field strength across the boundary, which is not continuous.

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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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