2 Problems regarding Gauss's Law

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SUMMARY

This discussion focuses on two problems related to Gauss's Law in electrostatics. The first problem involves calculating the electric field of a uniformly charged rod with a linear charge density of 6.5 x 10^-8 C/m, revealing that the electric field at a distance of 1 cm from the rod is significantly lower than that from a point charge of the same total charge. The second problem examines the motion of a negative point charge released from the surface of a uniformly charged solid sphere, leading to a description of simple harmonic motion with a period of 2π√(m/K) and conservation of total energy.

PREREQUISITES
  • Understanding of Gauss's Law and its application to electric fields
  • Familiarity with concepts of electric charge density and linear charge distribution
  • Knowledge of simple harmonic motion and its mathematical formulation
  • Ability to apply Coulomb's Law for point charges
NEXT STEPS
  • Study the derivation of electric fields using Gauss's Law for different charge distributions
  • Learn about the properties of simple harmonic motion and its energy conservation principles
  • Explore the concept of electric potential energy in electrostatics
  • Investigate the effects of charge distribution on electric fields in various geometries
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Students of physics, particularly those studying electromagnetism, educators teaching electrostatics, and anyone interested in the applications of Gauss's Law in real-world scenarios.

echau
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Hey everyone, I have two problems that deal with Gauss's law. The first one deals with Electric Fields.

Charge is distributed on a long, straight rod with uniform density 6.5 x 10^-8 C/m. Compare the magnitude of the field 1 cm from the rod to the field 1 cm from a point charge q = 6.5 x 10^-8.

The answer in the back of the book is: E(rod)/E(point)=.02=2%

I was thinking that the Electric fields would be the same since the charge is the same, but then I realized that the charge is spread out on the rod. How would I find the Field for the rod to solve the problem? I'm assuming that for the point charge it's just kq/r^2 = [(8.99 x 10^9)(6.5 x 10^-8)]/(.01^2).

The second problem is regarding motion.

Consider a solid sphere of radius R with a charge Q distributed uniformly. Suppose that a point charge q of mass m, with a sign opposite to that of Q, is free to move within a solid sphere. Charge q is placed at rest on the surface of the solid sphere and released. Describe the subsequent motion. In particular, what is the period of the motion, and what is the total energy of the point charge? [Hint: recall the properties of the motion for which the force varies linearly with the distance from a fixed point and is a restoring force.]

If anyone could help me with either of these two problems, I would greatly appreciate it. Thank you!
 
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Use Gauss law for the rod taking a coaxial cylinder of radius 1 cm as Guassian surface.
 
Thanks mukundpa!
You were right...the E(rod) is equal to (lamda)/[2(pi)(Epsilon)r]

I plugged in all the coefficients and it worked perfectly =)

Can anyone help me with the second problem?
 
For the second problem I think the charge distribution is volume charge distribution.
The charge density rho = Q/(4*PI*R^3/3)

Consider a spherical Guassion surface of radius x the charge within the Guassian surface will be rho*(4*PI*x^3/3) and hence fiels at distance x from the center will be
E(x) =rho*(4*PI*x^3/3)/eo*(4*Pi*x^2) = Q*x/(e0*4*Pi*R^3) which is proprtional to x

Now find the force actiong on the - ve charge and solve for simple harmonic motion.
 
So taking E = Q*x/(e0*4*Pi*R^3), I substitute that into E = F/q?

Therefore, F = Eq = Q*q*r/(e0*4*Pi*R^3)

Using F how would I obtain the total energy of the point charge? Period of motion?
Wouldn't the total energy be PE + KE?
I'm really not that good at Physics, can you explain the concept for me?
Thanks!
 
First of all the charge q is nigative so the force will be negetive ( atteractive) and towards the center of the sphere.

Secondaly q is released from the surface hence the amplitude is R, the radius of the sphere.

Thirdly if F = - Kx the time period is 2Pi*sq.rt.(m/K)

Total energy of the charge is only potential at the surface and remains conserved.
 
Thanks! I get it now.
 

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