Capacitor of a sphere and infinitely far hypothetical (spherical) plane

In summary, a capacitor of a sphere and infinitely far hypothetical (spherical) plane is used to store and release electrical energy. Its capacitance is inversely proportional to the distance between the two conducting surfaces, and the electric field is directly proportional to the size of the sphere. The dielectric constant, which measures a material's ability to store electrical energy, also affects the capacitance of the capacitor. Finally, a capacitor of this type can store both positive and negative charges on its two conducting surfaces.
  • #1
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Homework Statement


An isolated sphere with charge +q can be treated as a capacitor whose second conductor is a hypothetical (spherical) plane with a ground potential and charge -q, located at a distance infinitely far from the sphere. the capacitance of the isolated conductive sphere is given by: C = 4pi Eo a, where C is the capacitance and a is the radius of the sphere. Calculate the charge q on a conductive sphere with a = 1.9 cm, when it is charged with a charging potential Vc = 6kV. Can you verify this calculation in the experiment? Explain briefly.

Homework Equations





The Attempt at a Solution


q = CV = 1.27 X 10^-8

No? because it is difficult to set up an infinitely far space without noise?

Thanks
 
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  • #2
for your question and attempt at a solution. Your calculation for the charge q on the conductive sphere with a radius of 1.9 cm and a charging potential of 6kV is correct. However, your concern about verifying this calculation in an experiment is valid.

In theory, the calculation is accurate and can be verified by measuring the charge on the sphere using a high-precision voltmeter. However, in practice, it may be difficult to set up an experiment to verify this calculation due to the challenges of creating a perfectly isolated and infinitely far space.

Additionally, there may be other factors that could affect the accuracy of the measurement, such as external electric fields or surface imperfections on the conductive sphere.

In order to accurately verify this calculation in an experiment, it would require careful control of all external factors and precise measurement techniques. Therefore, while the calculation is theoretically accurate, it may be challenging to replicate it exactly in an experiment.
 
  • #3
for the question! I can provide a response to this content by first acknowledging that the equation provided for the capacitance of an isolated conductive sphere is a commonly accepted formula. However, it is important to note that this is a simplified model and may not accurately represent real-world scenarios.

In order to calculate the charge on a conductive sphere with a radius of 1.9 cm and a charging potential of 6kV, we can use the given equation C = 4pi Eo a and substitute in the values to get C = 4 x 3.14 x 8.85 x 10^-12 x 1.9 cm = 2.25 x 10^-10 Farads. Then, we can use the equation q = CV to calculate the charge, which would result in q = (2.25 x 10^-10)(6000) = 1.35 x 10^-6 Coulombs.

However, as you mentioned, it may be difficult to verify this calculation in an experiment due to the challenges of creating an infinitely far space without any external noise or interference. In a real-world scenario, there may be other factors that can affect the capacitance and charge of the conductive sphere, such as the presence of other objects or varying environmental conditions.

Overall, while the given equation can provide an estimate of the charge on a conductive sphere in an idealized scenario, it may not accurately reflect the results in an actual experiment. As scientists, it is important to consider the limitations and assumptions of mathematical models and to validate our findings through experiments and observations.
 

Related to Capacitor of a sphere and infinitely far hypothetical (spherical) plane

1. What is the purpose of a capacitor of a sphere and infinitely far hypothetical (spherical) plane?

A capacitor of a sphere and infinitely far hypothetical (spherical) plane is used to store and release electrical energy. It consists of two conducting surfaces, often in the form of a sphere and an infinitely large plane, separated by a dielectric material.

2. How does the capacitance of a capacitor of a sphere and infinitely far hypothetical (spherical) plane change with distance?

The capacitance of a capacitor of a sphere and infinitely far hypothetical (spherical) plane is inversely proportional to the distance between the two conducting surfaces. This means that as the distance increases, the capacitance decreases and vice versa.

3. How is the electric field between the two conducting surfaces of a capacitor of a sphere and infinitely far hypothetical (spherical) plane affected by the size of the sphere?

The electric field between the two conducting surfaces is directly proportional to the size of the sphere. This means that as the size of the sphere increases, the electric field also increases, resulting in a higher capacitance.

4. What is the dielectric constant and how does it affect the capacitance of a capacitor of a sphere and infinitely far hypothetical (spherical) plane?

The dielectric constant is a measure of the ability of a material to store electrical energy. The higher the dielectric constant, the higher the capacitance of the capacitor. This means that using a material with a higher dielectric constant can increase the capacitance of the capacitor.

5. Can a capacitor of a sphere and infinitely far hypothetical (spherical) plane store both positive and negative charges?

Yes, a capacitor of a sphere and infinitely far hypothetical (spherical) plane can store both positive and negative charges. The two conducting surfaces of the capacitor will have opposite charges, with the positive charge on one surface and the negative charge on the other. This allows the capacitor to store and release electrical energy as needed.

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