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An isolated large plate capacitor (not connected to anything) originally has a potential difference of 1000 V with an air gap of 2 mm. Then a plastic slab 1 mm thick, with dielectric constant 5, is inserted in the middle of the air gap as shown in figure 16.96. Calculate the following potential differences and explain your work.

V1-V2=?V2-V3=?V3-V4=?V1-V4=?

Short Answer

Expert verified

The potential difference between point 1 and 2 is 250 V, between point 2 and 3 is 100V , between point 3 and 4 is 250V and between point 1 and 4 is 600V .

Step by step solution

01

Identification of given data

The distance between plates of capacitor is l = 2 mm .

The potential difference across plates of capacitor is V = 1000 V .

The distance between point 1 and 2, point 3 and 4 is d = 0.5 mm

The thickness of plastic slab is t = 1 mm

The dielectric constant of plastic slab is k = 5

02

Conceptual Explanation

The potential difference for the air gap is calculated by the electric field multiplied by air gap. The potential difference for plastic slab is found by assuming slab dielectric material.

03

Determination of potential differences between given points

The electric field for air gap between plates is given as:

E=VIE=1000V2mm1m1000mmE=5×105V/m

The electric field for plastic slab between plates is given as:

Es=EKEs=5×105V/m5Es=1×105V/m

The electric potential between point 1 and point 2 is given as:

V2-V1=E.dV2-V1=5×105V/m0.5mm1m1000mmV2-V1=250V

The electric potential between point 2 and point 3 is given as:

V2-V3=Es.tV2-V3=1×105V/m1mm1m1000mV2-V3=100V

The electric potential between point 3 and point 4 is given as:

V3-V4=Es.dV3-V4=1×105V/m0.5mm1m1000mV3-V4=250V

The electric potential between point 1 and point 4 is given as:

V1-V4=V1-V2+V2-V3+(V3-V4)V1-V4=250V+100V+250VV1-V4=600V

Therefore, the potential difference between point 1 and 2 is 250V , between point 2 and 3 is 100V , between point 3 and 4 is 250V and between point 1 and 4 is 600V.

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Most popular questions from this chapter

The graph in Fig.16.56 shows the electric potential energy for a system of two interacting objects, as a function of the distance between the objects. What system might this graph represent?

(1) Two Protons, (2) Two sodium ions, (3) Two neutrons, (4) Two chloride ions, (5) Two electrons, (6) A Proton and an Electron, (7) A sodium ion and a chloride ion.

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.

Location A is a distance d from a charged particle. Location B is a distance 2d from the particle. Which of the following statements are true? It may help to draw a diagram. (1) If the charge of the particle is negative, VB-VAis negative. (2) If the charge of the particle is positive, (VA<VB). (3) If VB<VA, we know that the particle must be positive. (4) VB<VA, regardless of the sign of the charge of the particle. (5) The sign of(VB-VA)does not give us any information about the sign of the charge of the particle.

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?

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.

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