Electric field strength at a point between charges

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SUMMARY

The electric field strength at a point between two charges can be determined by setting the magnitudes of the electric fields due to each charge equal to each other. In this case, a +1.0 μC charge at point X and a +4.0 μC charge at point Y, 50 cm apart, create a scenario where the electric field is zero at a specific point along the line connecting them. By using the formula E = Q/4πε0r², the distances from each charge can be expressed as x for charge X and (0.5 - x) for charge Y. Solving the resulting equation will yield the exact location where the electric field strength is zero.

PREREQUISITES
  • Understanding of electric field concepts
  • Familiarity with Coulomb's law
  • Basic algebra for solving equations
  • Knowledge of the constant ε0 (permittivity of free space)
NEXT STEPS
  • Learn how to apply Coulomb's law in different configurations of charges
  • Study the concept of electric field lines and their implications
  • Explore the principle of superposition in electric fields
  • Investigate the effects of varying charge magnitudes on electric field strength
USEFUL FOR

Students studying electromagnetism, physics educators, and anyone interested in understanding electric fields and charge interactions.

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Homework Statement


A +1.0 μC charge is placed at point X. A +4.0 μC charge is placed at point Y,
50 cm from X.
How far from X, on the line XY, is the point where the electric field strength is zero?

Homework Equations


E = Q/4πε0r2

The Attempt at a Solution


I know that the electric field is zero at the point where the magnitude of the field due to the 1.0 μC charge is equal to the magnitude of the field due to the 4.0 μC charge, but I have tried making the equations equal to each other and don't know how to find r
 
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If you write up the equation the distances have to satisfy how does it look?
One hint is that if you define the distance from ##X## along the line as ##x## the distance from ##Y## can be written as ##(0.5-x)## (in meters).
 

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