15,000VIn the cathode ray tube found in old television sets, which contains a vacuum, electrons are boiled out of a very hot metal filament placed near a negative metal plate. These electrons start out nearly at rest and are accelerated toward a positive metal plate. They pass through a hole in the positive plate on their way toward the picture screen, as shown in the diagram in Figure 16.69. If the high-voltage supply in the television set maintains a potential difference of 15,000Vbetween the two plates, what speed do the electrons reach?

Short Answer

Expert verified

The final speed of the electron is 7.259×107m/s.

Step by step solution

01

Identification of given data

The potential difference between the two plates is, ΔV=15000V.

The distance between the two plates is, L.

02

Force acting on a moving charge

When a charge moves through a uniform electric field then an electric force acts on the charge.

The value of the electric force acting on the moving charge changes with the magnitude of the charge and the electric field.

03

Determining the velocity of the electron

The magnitude of the electric field acting between the two plates is given by,

E=ΔVL-kqL2=ΔVL

Here, kis Coulomb’s constant and its value is 9×109N·m2/C2.

Putting the values,

-9×109N·m2/C2-1.6×10-19CL2=15000VL1.44×10-9L2N·m2/C=15000VLL=1.44×10-9N·m2/C15000VL=9.6×10-14m

The force acting on the electron due to electric field is given by,

F=eEF=1.6×10-19C14.4×10-10L2N·m2/CF=23.04×10-29N·m29.6×10-14m2F=0.025N

Balancing the force using second law of motion,

F=mea

Here, ais the acceleration of the electron, and meis the mass of the electron, its value is 9.109×10-31kg.

Putting the values,

0.025N=9.109×10-31kg×aa=0.025N9.109×10-31kg×1kg·m/s21Na=2.75×1028m/s2

Using the equation of motion, the final speed of the electron is given by,

v2=u2+2asv2=0m/s2+22.75×1028m/s29.6×10-14mv2=5.269×1015m2/s2v=7.259×107m/s

Hence, the final speed of the electron is 7.259×107m/s.

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

In a circuit there is a copper wire 40 cm long with a potential difference from one end to the other end of 0.01V. What is the magnitude of electric field inside the wire?

Locations A, B and C are in a region of uniform electric field, as shown in the diagram in Figure 16.65. Location A is at -0.5,0,0m. Location B is at 0.5,0,0m. In the region the electric field has the value 750,0,0N/C. For a path starting at B and ending at A, calculate: (a) the displacement vector Δl, (b) the change in electric potential, (c) the potential energy change for the system when a proton moves from B to A, (d) the potential energy change for the system when an electron moves from B to A.

You travel along a path from location A to location B, moving in the same direction as the direction of the net electric field in that region. What is true of the potential difference VB-VA? (1) VB-VA>0, (2) VB-VA<0, (3) VB-VA=0.

long thin metal wire with radius rand lengthLis surrounded by a concentric long narrow metal tube of radius R, whereR>>L, as shown in Figure 16.86. Insulating spokes hold the wire in the center of the tube and prevent electrical contact between the wire and the tube. A variable power supply is connected to the device as shown. There is a charge+Qon the inner wire and a chargeQon the outer tube. As we will see when we study Gauss’s law in a later chapter, the electric field inside the tube is contributed solely by the wire, and the field outside the wire is the same as though the wire were infinitely thin; the outer tube does not contribute as long as we are not near the ends of the tube. (a) In terms of the chargeQ, lengthL, inner radiusr, and outer radiusR , what is the potential differenceVtubeVwire between the inner wire and the outer tube? Explain, and include checks on your answer. (b) The power-supply voltage is slowly increased until you see a glow in the air very near the inner wire. Calculate this power-supply voltage (give a numerical value), and explain your calculation. The lengthL=80 cm , the inner radiusr=0.7 mm, and the outer radiusR=3 cm. This device is called a “Geiger–Müller tube” and was one of the first electronic particle detectors. The voltage is set just below the threshold for making the air glow near the wire. A charged particle that passes near the center wire can trigger breakdown in the air, leading to a large current that can be easily measured.

2 Three charged metal disks are arranged as shown in Figure 16.75 (cutaway view). The disks are held apart by insulating supports not shown in the diagram. Each disk has an area of 2.5 m2 (this is the area of one flat surface of the disk). The charge Q1=5×10-8Cand the charge Q2=4×10-7C.

(a) What is the electric field (magnitude and direction) in the region between disks 1 and 2? (b) Which of the following statements are true? Choose all that apply. (1) Along a path from A to B, EΔI(2) VB-VA=0.(3) localid="1657088862802" VB-VA=-Q/2.5ε0+(0.003)V. . (c) To calculateVC-VB , where should the path start and where should it end? (d) Shouldlocalid="1657089209063" VC-VB be positive or negative? Why? (1) Positive, because localid="1657089087291" ΔIis opposite to the direction of . (2) Negative, becauseΔI is in the same direction asE . (3) Zero, becauseΔIE. (e) What is the potential differenceVC-VB ? (f) What is the potential differenceVD-VC ? (g) What is the potential differenceVF-VD ? (h) What is the potential differenceVG-VF ? (i) What is the potential differenceVG-VA? (j) The charged disks have tiny holes that allow a particle to pass through them. An electron that is traveling at a fast speed approaches the plates from the left side. It travels along a path from A to G. Since no external work is done on system of plates + electron, ΔK+ΔU=Wext=0. Consider the following states: initial, electron at location A; final, electron at location G. (1) What is the change in potential energy of the system? (2) What is the change in kinetic energy of the electron?

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