Concentric Cylindrical Conducting Shells

In summary: This means that the charge density on the outer shell must be doubled as well. Therefore, λouter,new = 2λouter,initial.
  • #1
maceng7
18
0

Homework Statement


The picture of the problem can be found here: http://www.2shared.com/photo/U_JIkDks/Capture.html

The questions that I'm having trouble with are:

(a) The magnitudes of the charge densities on the inner and outer shells are now changed (keeping λinner = -λouter) so that the resulting potential difference doubles (Vca,new = 2Vca,initial). How does Cnew, the capacitance of a one meter length of the system of conductors when the charge density is changed, compare to C, the initial capacitance of a one meter length of the system of conductors?

(b) What is λouter,new ?


Homework Equations



C = Q / ΔV
E = λ / 2∏rε
λ = Q/L

The Attempt at a Solution



(a) Alright for the first one I'm saying that the new capacitance will just equal the initial capacitance (before the charge densities were changed) because capacitance only depends on the geometry of the capacitor. If lambda is increased then that means the charges (Q) was increased, this increases the electric field which by this formula ΔV = Ed also increases the potential difference. Since the potential difference doubled, the total charge doubled (λ doubles) so the capacitance remains the same since it is only a ratio between the charge and potential difference.

(b) From above since potential difference doubled then λ must double as well so my new λ is 0.82μC/m

Does this seem correct? Thanks
 
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  • #2
maceng7 said:

Homework Statement


The picture of the problem can be found here: http://www.2shared.com/photo/U_JIkDks/Capture.html
The questions that I'm having trouble with are:

(a) The magnitudes of the charge densities on the inner and outer shells are now changed (keeping λinner = -λouter) so that the resulting potential difference doubles (Vca,new = 2Vca,initial). How does Cnew, the capacitance of a one meter length of the system of conductors when the charge density is changed, compare to C, the initial capacitance of a one meter length of the system of conductors?
Correct.


(b) What is λouter,new ?


Homework Equations



C = Q / ΔV
E = λ / 2∏rε
λ = Q/L

The Attempt at a Solution



(a) Alright for the first one I'm saying that the new capacitance will just equal the initial capacitance (before the charge densities were changed) because capacitance only depends on the geometry of the capacitor. If lambda is increased then that means the charges (Q) was increased, this increases the electric field which by this formula ΔV = Ed also increases the potential difference. Since the potential difference doubled, the total charge doubled (λ doubles) so the capacitance remains the same since it is only a ratio between the charge and potential difference.

(b) From above since potential difference doubled then λ must double as well so my new λ is 0.82μC/m

Does this seem correct? Thanks

Yes. Referring to a unit length of the cable, Q = CV, C hasn't changed so since V has doubled, so has Q.
 

Related to Concentric Cylindrical Conducting Shells

1. What is the purpose of using concentric cylindrical conducting shells?

The main purpose of using concentric cylindrical conducting shells is to provide a controlled electric field within the space between the two shells. This is useful in various electrical and electronic applications, such as capacitors and transmission lines.

2. How does the electric field behave between two concentric cylindrical conducting shells?

The electric field between two concentric cylindrical conducting shells is constant and uniform, meaning it has the same magnitude and direction at every point within the space between the shells. This is due to the fact that electric field lines are perpendicular to the surface of the conducting shells.

3. What is the relationship between the electric field and the potential difference between two concentric cylindrical conducting shells?

The electric field between two concentric cylindrical conducting shells is directly proportional to the potential difference between the two shells. This means that the stronger the electric field, the greater the potential difference between the shells.

4. Are there any practical limitations when using concentric cylindrical conducting shells?

Yes, there are practical limitations when using concentric cylindrical conducting shells. These include limitations on the size and shape of the shells, as well as the material used to make the shells. Additionally, the electric field between the shells can only be controlled up to a certain point before it starts to leak out into the surrounding environment.

5. How can concentric cylindrical conducting shells be used to shield against external electric fields?

Concentric cylindrical conducting shells can be used as a form of electromagnetic shielding, meaning they can block or reduce the impact of external electric fields. This is because the external electric field will induce a current on the outer shell, which will create an opposite electric field that cancels out the external field within the space between the shells.

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