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A spherical drop of water carrying a charge of \(30 \mathrm{pC}\) has a potential of \(500 \mathrm{~V}\) at its surface (with \(V=0\) at infinity). (a) What is the radius of the drop? (b) If two such drops of the same charge and radius combine to form a single spherical drop, what is the potential at the surface of the new drop?

Short Answer

Expert verified
The radius of the drop is 0.540 mm. The potential at the surface of the new drop is 478.7 V.

Step by step solution

01

Step 1

Identify the formula for the potential at the surface of a charged sphere. The potential \( V \) at the surface of a sphere with radius \( r \) carrying charge \( q \) is given by \[ V = \frac{kq}{r} \]where \( k = 8.99 \times 10^9 \, \text{Nm}^2/ \text{C}^2 \) is the Coulomb's constant.
02

Step 2

Rearrange the formula to solve for radius \( r \). Using the formula \( V = \frac{kq}{r} \), we solve for \( r \):\[ r = \frac{kq}{V} \]
03

Step 3

Substitute known values to calculate \( r \). Given \( V = 500 \, \text{V} \) and \( q = 30 \, \text{pC} = 30 \times 10^{-12} \, \text{C} \), substitute these values into the formula:\[ r = \frac{(8.99 \times 10^9)(30 \times 10^{-12})}{500} \approx 0.53994 \times 10^{-3} \text{m} \approx 0.540 \text{mm} \]
04

Step 4

Calculate the radius of the new drop from the volume formula. Since the volume must double when two identical droplets combine, use the volume equation for a sphere, \( V = \frac{4}{3}\pi r^3 \), to find the new radius:\[ 2 \left(\frac{4}{3}\pi r^3\right) = \frac{4}{3}\pi R^3 \]where \( R \) is the radius of the new combined drop.
05

Step 5

Solve for the new radius \( R \). From \[ 2r^3 = R^3 \],we find \[ R = 2^{1/3}r \approx 1.26r \] Substitute \( r \approx 0.540 \) mm, \[ R \approx 1.26 \times 0.540 \, \text{mm} = 0.6804 \, \text{mm} \]
06

Step 6

Calculate the potential at the new surface. Substitute \( R \) into the potential formula to find the new potential:\[ V' = \frac{k(60 \times 10^{-12})}{0.6804 \times 10^{-3}} \approx 478.7 \, \text{V} \]

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Key Concepts

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

Potential of Charged Sphere
Understanding the potential of a charged sphere is crucial in electrostatics. The potential (\( V \) ) at the surface of a charged sphere is determined by the charge (\( q \) ) it carries and the sphere's radius (\( r \) ). The formula used to calculate this is:\[ V = \frac{kq}{r} \]where \( k \) is the famous Coulomb's constant. This equation reveals that the potential is directly proportional to the charge and inversely proportional to the radius:
  • If the charge increases, the potential increases.
  • If the radius increases, the potential decreases.
Therefore, if you know the potential at the surface and the charge of the sphere, you can determine the sphere's radius. This is a typical scenario in problems where electrostatic phenomena are analyzed.
Coulomb's Constant
Coulomb's constant (\( k \) ) is a fundamental constant in physics, specifically in electrostatics. Its value is approximately \( 8.99 \times 10^9 \, \text{Nm}^2/ \text{C}^2 \) and it plays a key role in the calculations involving electric forces and fields.This constant is essential because it quantifies the magnitude of the electrostatic force between two point charges:\[ F = \frac{k |q_1 q_2|}{r^2} \]In the context of our exercise, Coulomb's constant appears in the formula to determine the electric potential of the sphere, showing its versatility. This constant allows precise calculations in a wide variety of applications, from the behavior of tiny water droplets to massive planetary and cosmic electric phenomena.
Volume of a Sphere
For a sphere, the volume (\( V \) ) is given by the formula:\[ V = \frac{4}{3}\pi r^3 \]This formula is pivotal when dealing with objects like droplets, where combining or dividing changes their attributes. When two identical spheres, or water droplets, merge, their combined volume is simply double the volume of one.In the exercise, knowing the relation:\[ 2 (\frac{4}{3}\pi r^3) = \frac{4}{3}\pi R^3 \]helps calculate the new radius (\( R \) ) of the combined sphere. This concept is significant because it shows how volume and radius are interrelated for spheres. The realization that \( R = 2^{1/3}r \) after combining droplets is crucial in solving the exercise efficiently.
Combining Charged Droplets
Combining two charged droplets means combining both their charges and volumes. The charges simply add up, so in this case, the new charge will be:\[ q' = 2q \]Often, however, the challenge lies in understanding how the potential changes. Initially, our drops each have a certain charge and radius. When they combine:
  • The new volume becomes twice the original, hence requiring recalculation of the radius.
  • The charge doubles, but due to the increased radius, the potential is lower than it might seem from a charge perspective alone.
To find the new potential, the expression \[ V' = \frac{kq'}{R} \] is used. As the radius increases, the potential at the surface does not simply double, emphasizing the intricate nature of electrostatic interactions among combined spheres.

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Most popular questions from this chapter

Two charges \(q=+2.0 \mu \mathrm{C}\) are fixed a distance \(d=2.0 \mathrm{~cm}\) apart (Fig. \(24-69\) ). (a) With \(V=0\) at infinity, what is the electric potential at point \(C ?\) (b) You bring a third charge \(q=+2.0 \mu \mathrm{C}\) from infinity to \(C .\) How much work must you do? (c) What is the potential energy \(U\) of the three charge configuration when the third charge is in place?

A particle of charge \(+7.5 \mu \mathrm{C}\) is released from rest at the point \(x=60 \mathrm{~cm}\) on an \(x\) axis. The particle begins to move due to the presence of a charge \(Q\) that remains fixed at the origin. What is the kinetic energy of the particle at the instant it has moved \(40 \mathrm{~cm}\) if (a) \(Q=+20 \mu \mathrm{C}\) and (b) \(Q=-20 \mu \mathrm{C} ?\)

An infinite nonconducting sheet has a surface charge density \(\sigma=0.10 \mu \mathrm{C} / \mathrm{m}^{2}\) on one side. How far apart are equipotential surfaces whose potentials differ by \(50 \mathrm{~V} ?\)

A charge of \(1.50 \times 10^{-8} \mathrm{C}\) lies on an isolated metal sphere of radius \(16.0 \mathrm{~cm} .\) With \(V=0\) at infinity, what is the electric potential at points on the sphere's surface?

Two isolated, concentric, conducting spherical shells have radii \(R_{1}=0.500 \mathrm{~m}\) and \(R_{2}=1.00 \mathrm{~m},\) uniform charges \(q_{1}=+2.00 \mu \mathrm{C}\) and \(q_{2}=+1.00 \mu \mathrm{C},\) and negligible thicknesses. What is the magnitude of the electric field \(E\) at radial distance (a) \(r=4.00 \mathrm{~m}\) (b) \(r=0.700 \mathrm{~m},\) and \((\mathrm{c}) r=0.200 \mathrm{~m} ?\) With \(V=0\) at infinity, what is \(V\) at \((\mathrm{d}) r=4.00 \mathrm{~m},(\mathrm{e}) r=1.00 \mathrm{~m},(\mathrm{f}) r=0.700 \mathrm{~m},(\mathrm{~g}) r=0.500 \mathrm{~m}\) (h) \(r=0.200 \mathrm{~m},\) and (i) \(r=0 ?(j)\) Sketch \(E(r)\) and \(V(r)\).

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