Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Two metal spheres are separated by a distance of \(1.0 \mathrm{cm}\) and a power supply maintains a constant potential difference of \(900 \mathrm{V}\) between them. The spheres are brought closer to one another until a spark flies between them. If the dielectric strength of dry air is $3.0 \times 10^{6} \mathrm{V} / \mathrm{m},$ what is the distance between the spheres at this time?

Short Answer

Expert verified
Answer: The distance between the spheres when the spark occurs is 0.3 mm or 3.0 x 10^-4 m.

Step by step solution

01

Find the electric field at the point where the spark occurs.

We can find the electric field at the point where the spark occurs by using the dielectric strength of dry air. The dielectric strength represents the maximum electric field that an insulating material, in this case, dry air, can withstand before breaking down. As a result, we can set the electric field at the point of the spark equal to the dielectric strength: \(E_{spark} = 3.0 \times 10^{6} \mathrm{\thinspace V/m}\)
02

Write down the formula for the electric field and potential difference.

The relationship between electric field and potential difference can be given as: \(V = E \times d\) Where: \(V\) is the potential difference between the two spheres, \(E\) is the electric field at a point in space, \(d\) is the distance between two points. We are given the potential difference between the spheres, \(V = 900 \mathrm{V}\), and we found the electric field at the point of the spark, \(E_{spark}\). Now we need to find the distance, \(d\), between the spheres at that point.
03

Solve for the distance between the spheres when the spark occurs.

Now let's substitute the values of the potential difference and the electric field into the formula and solve for the distance: \(900 \mathrm{V} = (3.0 \times 10^{6} \mathrm{V/m}) \times d\) To find the distance, we can divide both sides of the equation by \(3.0 \times 10^{6} \mathrm{V/m}\): \(d = \frac{900 \mathrm{V}}{3.0 \times 10^{6} \mathrm{V/m}}\) \(d = 3.0 \times 10^{-4} \mathrm{\thinspace m}\) So, the distance between the spheres when the spark occurs is \(3.0 \times 10^{-4} \mathrm{\thinspace m}\), or \(0.3 \mathrm{mm}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Figure 17.31 b shows a thundercloud before a lightning strike has occurred. The bottom of the thundercloud and the Earth's surface might be modeled as a charged parallel plate capacitor. The base of the cloud, which is roughly parallel to the Earth's surface, serves as the negative plate and the region of Earth's surface under the cloud serves as the positive plate. The separation between the cloud base and the Earth's surface is small compared to the length of the cloud. (a) Find the capacitance for a thundercloud of base dimensions \(4.5 \mathrm{km}\) by \(2.5 \mathrm{km}\) located \(550 \mathrm{m}\) above the Earth's surface. (b) Find the energy stored in this capacitor if the charge magnitude is \(18 \mathrm{C}\).
An electron is moved from point \(A\), where the electric potential is \(V_{A}=-240 \mathrm{V},\) to point \(B,\) where the electric potential is \(V_{B}=-360 \mathrm{V}\). What is the change in the electric potential energy?
(a) Calculate the capacitance per unit length of an axon of radius $5.0 \mu \mathrm{m} \text { (see Fig. } 17.14) .$ The membrane acts as an insulator between the conducting fluids inside and outside the neuron. The membrane is 6.0 nm thick and has a dielectric constant of \(7.0 .\) (Note: The membrane is thin compared with the radius of the axon, so the axon can be treated as a parallel plate capacitor.) (b) In its resting state (no signal being transmitted), the potential of the fluid inside is about \(85 \mathrm{mV}\) lower than the outside. Therefore, there must be small net charges \(\pm Q\) on either side of the membrane. Which side has positive charge? What is the magnitude of the charge density on the surfaces of the membrane?
A spherical conductor of radius \(R\) carries a total charge Q. (a) Show that the magnitude of the electric field just outside the sphere is \(E=\sigma / \epsilon_{0},\) where \(\sigma\) is the charge per unit area on the conductor's surface. (b) Construct an argument to show why the electric field at a point \(P\) just outside any conductor in electrostatic equilibrium has magnitude \(E=\sigma / \epsilon_{0},\) where \(\sigma\) is the local surface charge density. [Hint: Consider a tiny area of an arbitrary conductor and compare it to an area of the same size on a spherical conductor with the same charge density. Think about the number of field lines starting or ending on the two areas.]
A shark is able to detect the presence of electric fields as small as $1.0 \mu \mathrm{V} / \mathrm{m} .$ To get an idea of the magnitude of this field, suppose you have a parallel plate capacitor connected to a 1.5 - \(V\) battery. How far apart must the parallel plates be to have an electric field of $1.0 \mu \mathrm{V} / \mathrm{m}$ between the plates?
See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free