/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 7 A spherical drop of mercury of r... [FREE SOLUTION] | 91Ó°ÊÓ

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A spherical drop of mercury of radius \(R\) has a capacitance given by \(C=4 \pi \varepsilon_{0} R .\) If two such drops combine to form a single larger drop what is its capacitance?

Short Answer

Expert verified
The capacitance of the larger drop is \(4 \pi \varepsilon_0 R \sqrt[3]{2}\).

Step by step solution

01

- Understand the Initial Capacitance Formula

The initial capacitance of a spherical drop of mercury with radius \(R\) is given by the formula: \(C = 4 \pi \varepsilon_0 R\).
02

- Volume of the Spherical Drops

The volume of a single spherical drop is \(V = \frac{4}{3} \pi R^3\). Since there are two drops, their combined volume is \(2V = 2 \times \frac{4}{3} \pi R^3 = \frac{8}{3} \pi R^3\).
03

- Find the Radius of the Combined Drop

Let the radius of the new combined drop be \(R'\). The volume of the new drop must equal the combined volume of the original drops: \[ \frac{4}{3} \pi (R')^3 = \frac{8}{3} \pi R^3 \] Solving for \(R'\), we get \[ (R')^3 = 2R^3 \] \[ R' = R \sqrt[3]{2} \]
04

- Calculate the Capacitance of the New Drop

The capacitance of a spherical drop is \(C = 4 \pi \varepsilon_0 R'\). Substituting \(R'\) into this formula gives: \[ C' = 4 \pi \varepsilon_0 (R \sqrt[3]{2}) \] \[ C' = 4 \pi \varepsilon_0 R \sqrt[3]{2} \]

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Key Concepts

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

Electrostatics
Electrostatics is the branch of physics that studies electric charges at rest. In the context of this problem, electrostatics helps us understand the behavior of spherical drops of mercury and their capacitance.
Capacitance is a property that indicates how much electric charge a conductor can hold per unit voltage. For a spherical conductor, the capacitance is directly proportional to its radius. This relationship is given by the formula: \( C = 4 \pi \varepsilon_0 R \), where \( \varepsilon_0 \) is the permittivity of free space. Understanding this relationship is crucial for solving the problem of combining spherical drops and calculating the resulting capacitance.
Generally, in electrostatics, we deal with important parameters like electric field, electric potential, and capacitance. All these parameters help in defining and predicting the behavior of electric charges and fields in various scenarios.
Combining Drops
When two spherical drops combine, the total volume of the resulting drop is the sum of the volumes of the individual drops. For spherical drops of mercury, the volume of a single drop can be expressed as \(V = \frac{4}{3}\pi R^3\).
Let's assume we have two such drops. Their combined volume will be twice that of a single drop: \(2V = 2 \times \frac{4}{3}\pi R^3 = \frac{8}{3}\pi R^3\).
When these two drops merge, they form a new larger drop. To find the radius of the new drop, we equate its volume to the combined volume of the initial drops:
  • The volume equation: \( \frac{4}{3} \pi (R')^3 = \frac{8}{3} \pi R^3 \)
  • Solving for \( R' \) gives \((R')^3 = 2R^3\)
  • Taking the cube root gives \( R' = R \sqrt[3]{2} \)
This new radius is key for calculating the new capacitance.
Capacitance Calculation
The capacitance of a spherical drop is given by the formula: \( C = 4 \pi \varepsilon_0 R \). For the new combined drop with radius \( R' = R \sqrt[3]{2} \), we need to substitute this value into the capacitance formula:
\( C' = 4 \pi \varepsilon_0 (R \sqrt[3]{2}) \)
Breaking it down further:
\( C' = 4 \pi \varepsilon_0 R \sqrt[3]{2} \)
This formula indicates that the capacitance of the new drop is scaled by the factor \( \sqrt[3]{2} \) compared to a single drop of radius \( R \). This demonstrates how combining drops affects the capacitance, reflecting the direct proportionality of capacitance with radius in spherical conductors.
Volume Conservation
The principle of volume conservation states that the total volume remains constant when drops combine. For spherical drops of mercury in this problem, this means the total volume after combining is the sum of the individual volumes.
Each spherical drop has a volume given by \( V = \frac{4}{3}\pi R^3 \). When two drops combine, their total volume is: \( 2V = \frac{8}{3}\pi R^3 \).
This total volume must equate to the volume of the new larger drop, hence:\( \frac{4}{3}\pi (R')^3 = \frac{8}{3}\pi R^3 \). Simplifying this, we find: \( (R')^3 = 2R^3 \), thus \( R' = R \sqrt[3]{2} \).
Volume conservation plays a critical role in accurately determining the new radius, which then allows us to calculate the new capacitance accurately. This concept ensures consistency and precision in electrostatics problems involving spherical conductors.

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Most popular questions from this chapter

(a) What is the physical definition and description of a capacitor? (b) What is the mathematical definition of capacitance? (c) Based on the physical description of a capacitor, why would you expect it to hold more excess charge on each of its conducting surfaces when the voltage difference between the two pieces of conductor increases?

Shells The space between two concentric conducting spherical shells of radii \(b\) and \(a\) (where \(b>a\) ) is filled with a substance of dielectric constant \(\kappa .\) A potential difference \(\Delta V\) exists between the inner and outer shells. Determine (a) the capacitance of the device, (b) the excess free charge \(q\) on the inner shell, and (c) the charge \(q^{\prime}\) induced along the surface of the inner shell.

An air-filled parallel-plate capacitor has a capacitance of \(1.3 \mathrm{pF}\). The separation of the plates is doubled and wax is inserted between them. The new capacitance is \(2.6 \mathrm{pF}\). Find the dielectric constant of the wax.

A charged isolated metal sphere of diameter \(10 \mathrm{~cm}\) has a potential of \(8000 \mathrm{~V}\) relative to \(V=0\) at infinity. Calculate the energy density in the electric field near the surface of the sphere.

(a) Show that the plates of a parallel-plate capacitor attract each other with a force of magnitude given by \(F=q^{2} / 2 \varepsilon_{0} A .\) Do so by calculating the work needed to increase the plate separation from \(x\) to \(x+d x\), with the excess charge \(|q|\) remaining constant. (b) Next show that the magnitude of the force per unit area (the electrostatic stress) acting on either capacitor plate is given by \(\frac{1}{2} \varepsilon_{0} E^{2}\). (Actually, this is the force per unit area on any conductor of any shape with an electric field \(\vec{E}\) at its surface.)

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