Biology, asked by npafho70771, 1 year ago

Derive electric field inside and outside of a atom having nuclear charge ze?

Answers

Answered by raksha77
0

Explanation:

ved!

See the answer

An early model of the atom, proposed by Rutherford after his discovery of the atomic nucleus, had a positive point charge, +Ze (the nucleus) at the center of a sphere of radius R with uniformly distributed negative charge -Ze. Z is the atomic number, the number of protons in the nucleus and the number electrons in the negative sphere.

Estimate the charged enclosed within a sphere with the nucleus at its center, and the radius of r, smaller than R.

Use Gauss' law to obtain the electric field inside this atom.

A uranium atom has Z = 92 and R = 0.10 nm. Estimate the electrostatic force that an electron would experience at r = R/2?

Assuming that the electron in c) is in the uniform circular motion around the nuclear, estimate the speed of the electron.

What is the electric field outside the atom? Explain your result.

The electric potential energy at a certain position is defined as the amount of work by the electric force, needed to bring a charge from the infinite to the position. Estimate the potential energy of the electron, considered in

c), at r = R/2 in the uranium atom.

Estimate the electric potential at r = R/2.

Answered by Anonymous
1

→p = 

−→d

where −→d points from the negative to positive charge.

The concept of electric potential is especially useful for

calculating the electric field for the electric dipole.

The electric potential relative to infinity at the

point  in a figure 1 is given by:

 = 1

4

Ã

£

 − ¡ 

2

¢

cos 2

¤ − 

£

 + ¡ 

2

¢

cos 1

¤

!

where 2 is the angle for the positive charge and 1 for

the negative charge. Let    then 1 ≈ 2 ≈ ,

and the equation simplifies to:

 = 

4

 cos 

h

2 − ¡ 

2

¢2

cos2 

i ' 

4

 cos 

2

The electric dipole moment is given by:

−→p =bi

that is, the electric dipole moment is a vector quantity

as opposed to the monopole moment .

Thus the electric potential relative to infinity can

be written as:

 =

−→p · br

42   

since bi·br = cos  where br point from the electric dipole

towards the point .

Similar questions