An electron is released from rest just above a very large, negatively charged sheet, which carries surface charge density \(\sigma=5 \mathrm{nC} / \mathrm{m}^2\). When the electron is \(0.5 \mathrm{~m}\) above the sheet its speed is most nearly (A) \(4 \times 10^8 \mathrm{~m} / \mathrm{s}\) (B) \(3 \times 10^8 \mathrm{~m} / \mathrm{s}\) (C) \(5 \times 10^7 \mathrm{~m} / \mathrm{s}\) (D) \(1 \times 10^7 \mathrm{~m} / \mathrm{s}\) (E) \(300 \mathrm{~m} / \mathrm{s}\)

Short Answer

Expert verified
Answer: (C) \(5 \times 10^7 \mathrm{m} / \mathrm{s}\)

Step by step solution

01

Calculate the Electric Field produced by the charged sheet

The electric field produced by an infinite sheet with a surface charge density \(\sigma\) is given by:$$E = \frac{\sigma}{2\epsilon_0}$$Where \(\epsilon_0\) is the vacuum permittivity (\(8.85 × 10^{-12} \mathrm{C^2} / \mathrm{N m^2}\)). Now we can calculate the electric field produced by the charged sheet. Substitute the surface charge density (\(\sigma = 5 \times 10^{-9} \mathrm{C/m^2}\)) into the equation:$$E = \frac{5 \times 10^{-9}}{2 \times 8.85 \times 10^{-12}}$$
02

Calculate the Force acting on the Electron

Force acting on the electron due to the electric field is given by:$$F = qE$$Where \(q\) is the charge of the electron, which is \(q = -1.6 \times 10^{-19} \mathrm{C}\). Now, we can calculate the force acting on the electron. Substitute the charge of the electron and the electric field calculated in Step 1 into the equation:$$F = (-1.6 \times 10^{-19})\left(\frac{5 \times 10^{-9}}{2 \times 8.85 \times 10^{-12}}\right)$$
03

Calculate the Work Done on the Electron

Work done on the electron is given by:$$W = Fd$$Where \(d\) is the distance the electron traveled, which is \(0.5 \mathrm{m}\). Now we can calculate the work performed on the electron using the force calculated in Step 2 and the distance:$$W = \left((-1.6 \times 10^{-19})\left(\frac{5 \times 10^{-9}}{2 \times 8.85 \times 10^{-12}}\right)\right)(0.5)$$
04

Calculate the Change in Kinetic Energy of the Electron

The work-energy theorem states that the work done on an object is equal to the change in its kinetic energy. Therefore, we can write:$$\Delta K = W$$Now we can find the change in kinetic energy of the electron using the work calculated in Step 3:$$\Delta K = \left((-1.6 \times 10^{-19})\left(\frac{5 \times 10^{-9}}{2 \times 8.85 \times 10^{-12}}\right)\right)(0.5)$$
05

Calculate the Final Velocity of the Electron

The kinetic energy of the electron is given by:$$K = \frac{1}{2}mv^2$$Where \(m\) is the mass of an electron, which is \(9.11 \times 10^{-31} \mathrm{kg}\), and \(v\) is its speed. We have the change in kinetic energy, so we can calculate the final velocity of the electron. Rearrange the equation for kinetic energy and solve for the final velocity:$$v = \sqrt{\frac{2\Delta K}{m}}$$Substitute the mass of the electron and change in kinetic energy into the equation:$$v = \sqrt{\frac{2\left((-1.6 \times 10^{-19})\left(\frac{5 \times 10^{-9}}{2 \times 8.85 \times 10^{-12}}\right)\right)(0.5)}{9.11 \times 10^{-31}}}$$ Calculate the final value for the velocity of the electron. The answer is closest to (C) \(5 \times 10^7 \mathrm{m} / \mathrm{s}\).

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Most popular questions from this chapter

Proton \(A\) is moving with speed \(10^6 \mathrm{~m} / \mathrm{s}\) in a magnetic field of \(0.01 \mathrm{~T}\). Proton \(B\) is moving in the same magnetic field with speed \(2 \times 10^6 \mathrm{~m} / \mathrm{s}\). One can conclude that (A) Both protons have an orbital radius of about 1 meter. (B) Both protons have the same orbital period of about \(6.5 \times 10^{-6} \mathrm{~s}\). (C) proton \(B\) has twice the orbital period of proton \(A\). (D) proton \(B\) has twice the orbital frequency of proton \(A\). (E) proton \(B\) has half the orbital radius of proton \(B\).

The below fields represent electric or magnetic fields associated with a long current-carrying wire, a single positive charge, two oppositely charged particles, two positive charges, and the field between two oppositely charged parallel sheets. (A) A, D, C, B, E (B) E, A, D, C, B (C) E, D, A, B, C (D) D, E, C, B, A (E) C, B, A, E, D

Until recently, TV sets consisted of what was called a cathode-ray tube. Electrons were boiled off a light bulb filament and passed through plates that deflected the particles; the electron beam went on to strike the TV screen itself and lit up a pixel of phosphor. The beam could be deflected both up and down and sideways (only one direction shown). By deflecting the electron beam and scanning it across the screen a picture was built up. Consider the simplified TV below. An electron beam is shot along the centerline between the two deflector plates. The top plate is held by a power supply (not shown) at a voltage \(V=\) \(+1000\) volts above the bottom plate. The separation between the plates is \(d=4 \mathrm{~cm}\). The length of the plates is \(\ell=8 \mathrm{~cm}\). The distance \(L\) from the end of the deflector plate to the TV screen is \(30 \mathrm{~cm}\). The electrons enter the region between the deflector plates with a velocity \(v=4 \times 10^7 \mathrm{~m} / \mathrm{s}\). a) In which direction is the electric field between the deflector plates? b) In which direction are the electrons deflected? c) What is the force on an electron? (Neglect gravity.) d) What is the acceleration on the electron? e) What is the total deflection of the electron as it hits the TV screen? f) What size magnetic field and in what direction would you need to place between the deflector plates in order to prevent the electrons from being deflected?

Two conducting spheres of differing radii are in contact, as shown. A positively charged rod is touched to the large sphere and removed to a great distance. The large and small spheres are then separated. We can then say that (A) the big sphere will be positively charged and the smaller sphere will be negatively charged. (B) both spheres will be positively charged. (C) the big sphere will be negatively charged and the smaller sphere will be positively charged. (D) both spheres will be negatively charged. (E) all the charge will migrate to the smaller sphere.

The positively charged rod is brought near the large sphere, but without touching it. The two spheres are separated and lastly the rod removed to a distance. We can then say that (A) the big sphere will be positively charged and the smaller sphere will be negatively charged. (B) both spheres will be positively charged. (C) the big sphere will be negatively charged and the smaller sphere will be positively charged. (D) both spheres will be negatively charged. (E) all the charge will migrate to the smaller sphere.

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