How Does Charge Distribution Affect Electric Field Magnitude?

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SUMMARY

The discussion focuses on calculating the electric field magnitude at the point (b, 0) due to two point charges, Q and -Q, positioned at (0, a) and (0, -a) respectively. The derived formula for the electric field is E = Qa / [2πε0(a²+b²)^(3/2)], where ε0 is the permittivity of free space, valued at 8.85 x 10^-12. The participants emphasize the importance of vector direction and the need for a diagram to resolve forces accurately, particularly regarding the angle x between the resultant electric fields and the x-axis.

PREREQUISITES
  • Understanding of electric fields and point charges
  • Familiarity with vector addition in physics
  • Knowledge of trigonometric functions (sine and cosine)
  • Basic principles of electrostatics, including Coulomb's law
NEXT STEPS
  • Study the derivation of electric field equations in electrostatics
  • Learn about vector components and their significance in physics
  • Explore the concept of electric field lines and their graphical representation
  • Investigate the implications of charge distribution on electric field strength
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Students in physics, particularly those studying electromagnetism, educators teaching electric field concepts, and anyone interested in the mathematical modeling of electric fields due to point charges.

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Homework Statement



The x-y plane contains point charge with magnitudes and positions as follows:

A charge of Q lies at co-ordinates (0, a)
A charge of -Q lies at co-ordinates (0,-a)

Show that the magnitude of the electric field at (b, 0) is given by

E = Qa / [2πε0(a²+b²)^(3/2)]

ε0 = Epsilon nought = 8.85 x10^-12


Homework Equations



E = Q/ 4πε0r²

The Attempt at a Solution



E due to Q is

E1 = Q/ 4πε0r²
E1 = Q/ 4πε0(a²+b²)

Therefore the vector E'

E' = E1*Cos(x) i^ + E1*Sin(x) j^
E' = QCos(x) / 4πε0(a²+b²) i^ + QSin(x)/ 4πε0(a²+b²) j^

E due to -Q is

E2 = Q/ 4πε0r²
E2 = Q/ 4πε0(a²+b²)

Therefore the vector E''

E'' = E2*Cos(x) i^ + E2*Sin(x) j^
E'' = QCos(x) / 4πε0(a²+b²) i^ + QSin(x)/ 4πε0(a²+b²) j^

Vector E = E' + E''
E = QCos(x) / 4πε0(a²+b²) i^ + QSin(x)/ 4πε0(a²+b²) j^
+ QCos(x) / 4πε0(a²+b²) i^ + QSin(x)/ 4πε0(a²+b²) j^
E = QCos(x) / 2πε0(a²+b²) i^ + QSin(x)/ 2πε0(a²+b²) j^

Magnitude of E
E = sqrt{Q²Cos²(x) / [2πε0(a²+b²)]² + Q²Sin²(x)/ [2πε0(a²+b²)]²}

E = Q / 2πε0(a²+b²)

As you can see its close lol, need Q*a not Q by itself and (a²+b²) should be(a²+b²)^(3/2)?
 
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remember that one charge is +Q and another is -Q. Also remember that electric fields are vectors and therefore direction matters, so your use of "cos(x)" and "sin(x)" in both equations begs the question "what is x referring to here?" So, my advice is to draw a diagram. It will make the question much simpler.
 
Sorry i forgot to explain what x is. After drawing a diagram with resolved forces at (b,0), x would be the angle between the resultant E fields and the x axis. I am not sure which signs need to be negative any clues/advice/lecture will be appreciated very much.
 

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