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Suppose that an electron inside a cathode ray tube starts from rest and is accelerated by the tube's voltage of \(21.9 \mathrm{kV}\). What is the speed (in \(\mathrm{km} / \mathrm{s}\) ) with which the electron (mass \(\left.=9.11 \cdot 10^{-31} \mathrm{~kg}\right)\) hits the screen of the tube?

Short Answer

Expert verified
Given the mass of an electron is \(9.11 \times 10^{-31} \mathrm{kg}\). Answer: To find the speed of the electron, follow the given steps and calculate the value of \(v\): $$v = \sqrt{\frac{2((-1.60 \times 10^{-19} \mathrm{C})(21.9 \times 10^3 \mathrm{V}))}{9.11 \times 10^{-31} \mathrm{kg}}}$$ Then, convert the final velocity to km/s using: $$v_{km/s} = v_{m/s} \frac{1}{1000}$$

Step by step solution

01

Identify known quantities

The known quantities in this problem are: - Electron mass: \(m = 9.11 \times 10^{-31} \mathrm{kg}\) - Voltage across the tube: \(V = 21.9 \times 10^3 \mathrm{V}\)
02

Use the work-energy theorem

The work-energy theorem states that the work done on an object is equal to the change in its kinetic energy. In this case, the work done on the electron by the electric force is equal to the change in the electron's kinetic energy: $$W = \Delta KE$$
03

Relate work, charge, and voltage

The work done on an object by an electric force is equal to the product of the charge of the object and the voltage through which the charge is moved: $$W = qV$$ For an electron, the charge is \(q = -e = -1.60 \times 10^{-19} \mathrm{C}\). Therefore, the work done on the electron is $$W = (-1.60 \times 10^{-19} \mathrm{C})(21.9 \times 10^3 \mathrm{V})$$
04

Calculate the change in kinetic energy

From steps 2 and 3, we can now calculate the change in the electron's kinetic energy: $$\Delta KE = (-1.60 \times 10^{-19} \mathrm{C})(21.9 \times 10^3 \mathrm{V})$$
05

Determine the final velocity

The kinetic energy of an object depends on its mass and velocity as follows: $$KE = \frac{1}{2} m v^2$$ Since the electron starts from rest, the initial kinetic energy is zero, and the change in kinetic energy is equal to the final kinetic energy: $$\Delta KE = \frac{1}{2} m v^2$$ Now, we can solve for the final velocity \(v\) using the equation above and the values calculated in previous steps: $$v^2 = \frac{2 \Delta KE}{m}$$ $$v = \sqrt{\frac{2((-1.60 \times 10^{-19} \mathrm{C})(21.9 \times 10^3 \mathrm{V}))}{9.11 \times 10^{-31} \mathrm{kg}}}$$ Calculate the value of \(v\).
06

Convert the final velocity to km/s

After calculating the speed of the electron in meters per second, take the value of \(v\) and convert it to kilometers per second: $$v_{km/s} = v_{m/s} \frac{1}{1000}$$ This will give the final speed of the electron in km/s.

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Most popular questions from this chapter

A point charge \(Q\) is placed a distance \(R\) from the center of a conducting sphere of radius \(a\), with \(R>a\) (the point charge is outside the sphere). The sphere is grounded, that is, connected to a distant, unlimited source and/or sink of charge at zero potential. (Neither the distant ground nor the connection directly affects the electric field in the vicinity of the charge and sphere.) As a result, the sphere acquires a charge opposite in sign to \(Q\), and the point charge experiences an attractive force toward the sphere. a) Remarkably, the electric field outside the sphere is the same as would be produced by the point charge \(Q\) plus an imaginary mirror-image point charge \(q\), with magnitude and location that make the set of points corresponding to the surface of the sphere an equipotential of potential zero. That is, the imaginary point charge produces the same field contribution outside the sphere as the actual surface charge on the sphere. Calculate the value and location of \(q\). (Hint: By symmetry, \(q\) must lie somewhere on the axis that passes through the center of the sphere and the location of \(Q .)\) b) Calculate the force exerted on point charge \(Q\) and directed toward the sphere, in terms of the original quantities \(Q, R\), and \(a\). c) Determine the actual nonuniform surface charge distribution on the conducting sphere.

A ring with charge \(Q\) and radius \(R\) is in the \(y z\) -plane and centered on the origin. What is the electric potential a distance \(x\) above the center of the ring? Derive the electric field from this relationship.

The amount of work done to move a positive point charge \(q\) on an equipotential surface of \(1000 \mathrm{~V}\) relative to that done to move the charge on an equipotential surface of \(10 \mathrm{~V}\) is a) the same. b) less. c) more. d) dependent on the distance the charge moves.

If a proton and an alpha particle (composed of two protons and two neutrons) are each accelerated from rest through the same potential difference, how do their resulting speeds compare? a) The proton has twice the speed of the alpha particle. b) The proton has the same speed as the alpha particle. c) The proton has half the speed of the alpha particle. d) The speed of the proton is \(\sqrt{2}\) times the speed of the alpha particle. e) The speed of the alpha particle is \(\sqrt{2}\) times the speed of the proton.

A \(2.50-\mathrm{mg}\) dust particle with a charge of \(1.00 \mu \mathrm{C}\) falls at a point \(x=2.00 \mathrm{~m}\) in a region where the electric potential varies according to \(V(x)=\left(2.00 \mathrm{~V} / \mathrm{m}^{2}\right) x^{2}-\left(3.00 \mathrm{~V} / \mathrm{m}^{3}\right) x^{3} .\) With what acceleration will the particle start moving after it touches down?

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