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24.13. A spherical capacitor contains a charge of 3.30 \(\mathrm{nC}\) when connected to a potential difference of 220 \(\mathrm{V}\) . If its plates are sepa- rated by vacuum and the inner radius of the outer shell is \(4.00 \mathrm{cm},\) calculate: (a) the capacitance; (b) the radius of the inner sphere; (c) the electric field just outside the surface of the inner sphere.

Short Answer

Expert verified
a) 15.0 pF, b) 3.5 cm, c) \(2.61 \times 10^4\, \mathrm{N/C}\).

Step by step solution

01

Understanding Capacitance in Spherical Capacitors

The capacitance for a spherical capacitor, with an inner sphere radius of \(r_1\) and outer sphere radius of \(r_2\), is given by:\[C = \frac{4\pi\varepsilon_0 r_1r_2}{r_2-r_1}\]where \(\varepsilon_0\) is the permittivity of free space, \(\varepsilon_0 \approx 8.85 \times 10^{-12}\, \frac{F}{m}\). We will use this formula to solve for specific values.
02

Calculate the Capacitance

Given the charge \(Q = 3.30\, \mathrm{nC} = 3.30 \times 10^{-9}\, \mathrm{C}\) and the potential difference \(V = 220\, \mathrm{V}\), the capacitance \(C\) is calculated using:\[C = \frac{Q}{V}\]Plugging in the values:\[C = \frac{3.30 \times 10^{-9}}{220} \approx 1.50 \times 10^{-11}\, \mathrm{F}\]
03

Rearrange the Capacitance Formula to Find Inner Radius

Using the capacitance formula from Step 1:\[C = \frac{4\pi\varepsilon_0 r_1r_2}{r_2-r_1}\]Rearrange this to solve for \(r_1\):\[r_1 = \frac{Cr_2}{4\pi\varepsilon_0 r_2 + Cr_2/C}\]Given \(r_2 = 4.00\, \mathrm{cm} = 0.04\, \mathrm{m}\), substitute known values and solve.
04

Calculate the Inner Radius

Substituting known quantities into the rearranged equation for \(r_1\):\[r_1 = \frac{1.50 \times 10^{-11} \times 0.04}{4\pi \times 8.85 \times 10^{-12} \times 0.04 + (1.50 \times 10^{-11})} \]After solving, \(r_1\) is approximately calculated, leading to:\[r_1 = 0.035\, \mathrm{m} = 3.5\, \mathrm{cm}\]
05

Calculate the Electric Field on the Inner Sphere's Surface

The electric field \(E\) just outside the inner sphere is given by:\[E = \frac{Q}{4\pi\varepsilon_0 r_1^2}\]Substitute for \(Q = 3.30 \times 10^{-9}\, \mathrm{C}\) and \(r_1 = 0.035\, \mathrm{m}\):\[E = \frac{3.30 \times 10^{-9}}{4\pi \times 8.85 \times 10^{-12} \times (0.035)^2}\]Calculating gives \(E\approx 2.61 \times 10^4\, \mathrm{N/C}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Capacitance Calculation
When dealing with spherical capacitors, it is essential to understand how capacitance is determined by the geometry of the capacitor and the properties of the material between its plates. The capacitance of a spherical capacitor can be calculated if the radii of the inner and outer spheres and the permittivity of the material between them are known.
For a spherical capacitor, the formula for capacitance is:
  • \( C = \frac{4\pi\varepsilon_0 r_1r_2}{r_2-r_1} \)
where \( r_1 \) is the radius of the inner sphere, \( r_2 \) is the radius of the outer sphere, and \( \varepsilon_0 \) is the permittivity of free space, approximately \( 8.85 \times 10^{-12}\, \mathrm{F/m} \).

In practice, once you know the charge \( Q \) on the capacitor and the potential difference \( V \) across it, you can compute the capacitance using \( C = \frac{Q}{V} \). This relation allows us to link the electrical properties directly to the measurable physical characteristics of the system. In our particular problem, with the given charge of 3.30 nC and a voltage of 220 V, the capacitance calculation yields \( 1.50 \times 10^{-11} \mathrm{F} \).
Electric Field
The electric field in a spherical capacitor is crucial because it helps to understand the distribution of force around the charged bodies. After we have calculated the capacitance, the next step is to calculate the electric field just outside the surface of the inner sphere.

The electric field \( E \) at a distance from a point charge is given by:
  • \( E = \frac{Q}{4\pi\varepsilon_0 r_1^2} \)
where \( Q \) is the charge and \( r_1 \) is the radius of the inner sphere. This formula is derived from Gauss's law, which addresses how an electric field emanates from a charged body.
For our specific problem, with a charge of 3.30 nC and an inner radius of 0.035 m, the electric field is determined to be approximately \( 2.61 \times 10^4 \mathrm{N/C} \). This calculation provides insight into the force experienced by a hypothetical 1 C charge placed just outside the inner sphere.
Inner and Outer Radius Calculation
Knowing the radii of the inner and outer parts of a spherical capacitor is essential for calculating both the capacitance and understanding the capacitor's spatial configuration.

To find the inner radius \( r_1 \), we manipulate the capacitance formula:
  • \( r_1 = \frac{Cr_2}{4\pi\varepsilon_0 r_2 + Cr_2/C} \)
This rearrangement allows calculation of the inner radius if the outer radius and capacitance are known.
In the given exercise, the outer radius \( r_2 \) is specified as 4.00 cm \((0.04 \mathrm{m})\). Substituting the values, we derive the inner radius \( r_1 \) to be about 3.5 cm. The accurate determination of these radii assists in applying the theoretical formulae accurately, ensuring a correct physical understanding of a spherical capacitor's behavior in real situations.

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Most popular questions from this chapter

24.6. A \(10.0-\mu F\) parallel-plate capacitor is connected to a \(12.0-\mathrm{V}\) battery. After the capacitor is fully charged, the battery is disconnected without loss of any of the charge on the plates. (a) A voltmeter is connected across the two plates without discharging them. What does it read? (b) What would the voltmeter read if ( i) the plate separation were doubled; (ii) the radius of each plate were doubled and, but their separation was unchanged?

24.4. Capacitance of an Oscilloscope. Oscilloscopes have parallel metal plates inside them to deflect the electron beam. These plates are called the deflecting plates. Typically, they are squares 3.0 \(\mathrm{cm}\) on a side and separated by \(5.0 \mathrm{mm},\) with vacuum in between. What is the capacitance of these deflecting plates and hence of the oscilloscope? (Note: This capacitance can sometimes have an effect on the circuit you are trying to study and must be taken into consideration in your calculations.)

24.21. Two parallel-plate vacuum capacitors have areas \(A_{1}\) and \(A_{2}\) and equal plate spacings \(d .\) Show that when the capacitors are connected in parallel, the equivalent capacitance is the same as for a single capacitor with plate area \(A_{1}+A_{2}\) and spacing \(d\) .

24.29. A parallel-plate vacuum capacitor with plate area \(A\) and separation \(x\) has charges \(+Q\) and \(-Q\) on its plates. The capacitor is disconnected from the source of charge, so the charge on each plate remains fixed. (a) What is the total energy stored in the capacitor? (b) The plates are pulled apart an additional distance \(d x\) . What is the change in the stored energy? (c) If \(F\) is the force with which the plates attract each other, then the change in the stored energy must equal the work \(d W=F d x\) done in pulling the plates apart. Find an expression for \(F\) (d) Explain why \(F\) is not equal to \(Q E\) , where \(E\) is the electric field between the plates.

24.28. A capacitor of capacitance \(C\) is charged to a potential difference \(V_{0}\) . The terminals of the charged capacitor are then connected to those of an uncharged capacitor of capacitance \(C / 2\) Compute (a) the original charge of the system; (b) the final potential difference across each capacitor; (e) the final energy of the system; (d) the decrease in energy when the capacitors are connected. (e) Where did the "lost" energy go?

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