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A gold nucleus has a radius of 7.3 \(\times 10^{-15}\) m and a charge of \(+79e\). Through what voltage must an alpha particle, with charge \(+2e\), be accelerated so that it has just enough energy to reach a distance of 2.0 \(\times 10^{-14}\) m from the surface of a gold nucleus? (Assume that the gold nucleus remains stationary and can be treated as a point charge.)

Short Answer

Expert verified
The voltage required is approximately 8.34 MV.

Step by step solution

01

Understanding the Problem

We need to determine the voltage required to accelerate an alpha particle to a specific distance from a gold nucleus. The nucleus is treated as a point charge with a charge of \(+79e\). The initial and final distances from the center of the nucleus should be calculated in order to apply the concept of potential difference.
02

Calculating Initial and Final Distances

Since the alpha particle ends up at 2.0 \(\times 10^{-14}\) m from the surface of the gold nucleus, and the radius of the nucleus is 7.3 \(\times 10^{-15}\) m, the final distance from the center of the nucleus is \(r_f = 2.0 \times 10^{-14} + 7.3 \times 10^{-15} = 2.73 \times 10^{-14}\) m. The initial distance \(r_i\) is effectively infinite as the particle starts far away.
03

Applying Potential Energy Formula

The potential energy \(U\) of a charge \(q\) at a distance \(r\) from a point charge \(Q\) is given by \(U = \frac{kQq}{r}\). Substituting \(Q = +79e\) and \(q = +2e\), the potential energies at \(r_i\) and \(r_f\) are calculated.
04

Determining the Potential Difference

The potential difference (voltage) needed to achieve the desired separation can be found using \(V = \frac{kQ}{r}\). The change in potential energy \(\Delta U = U_f - U_i\) must equal the kinetic energy imparted to the alpha particle.
05

Calculating the Voltage

Using \(e = 1.6 \times 10^{-19}\) C and \(k = 8.99 \times 10^9\) N m²/C², calculate the voltage:\[V = \frac{k \cdot 79e \cdot 2e}{2.73 \times 10^{-14}}\]This gives \[V = \frac{(8.99 \times 10^9) \, (79) \, (2) \, (1.6 \times 10^{-19})^2}{2.73 \times 10^{-14}} \approx 8.34 \, \text{M}V\]
06

Conclusion

The required voltage is approximately 8.34 MV. This means the alpha particle must be accelerated through a potential difference of 8.34 million volts to reach the specified distance from the gold nucleus.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Electric Potential Energy
Electric potential energy is a form of energy associated with the position of a charged particle in an electric field.
This concept is integral to understanding how alpha particles interact with gold nuclei. When a charge is moved within an electric field, it gains or loses electric potential energy.
The potential energy, denoted as \( U \), between two point charges is calculated using the formula:
  • \( U = \frac{kQq}{r} \), where:
  • \( k \) is Coulomb's constant \( (8.99 \times 10^9 \text{ N m}^2/ ext{C}^2) \)
  • \( Q \) and \( q \) represent the charges
  • \( r \) is the distance between the charges.

This energy concept answers why a voltage is needed to move an alpha particle to a specific point relative to another charged entity such as a gold nucleus.
It's the difference in electrical potential that contributes to the energy required for movement through an electric field.
Point Charge
A point charge is an idealized model where a charged object is assumed to be concentrated at a single point in space.
This simplification makes it easier to analyze the interactions between charges. In your exercise, the gold nucleus is treated as a point charge despite its actual physical size. Treating larger objects as point charges allows us to use simple equations, like Coulomb’s Law, without accounting for specific charge distribution. It also makes calculations manageable, especially when dealing with very small distances or very high charges.This implies that the gold nucleus, with a charge of \(+79e\), acts like a single concentrated charge that influences other charges, such as the \(+2e\) of an alpha particle, according to the rules of electrostatic interaction.
This assumption holds true mostly under cases where the position of interest is significantly farther from the nucleus compared to its size.
Alpha Particle
An alpha particle is a type of ionizing particle that consists of two protons and two neutrons bound together.
It is positively charged due to its pair of protons, carrying a charge of \(+2e\). This is a key component in nuclear reactions and radioactive decay processes.In this exercise, the alpha particle's positive charge makes it repelled by the similarly charged gold nucleus.
Hence, to overcome this repulsive force and bring the alpha particle close to the gold nucleus, the particle must be accelerated. Alpha particles are considerably more massive than electrons, meaning they require larger energies or voltages to achieve high velocities.
For a nuclear physics computation, accounting for their interaction with nuclear fields like that of the gold nucleus is essential.
Kinetic Energy
Kinetic energy is the energy that a body possesses due to its motion. In classical mechanics, this is given by:
  • \( KE = \frac{1}{2}mv^2 \)
  • Where \( m \) is mass
  • \( v \) is velocity.

For charged particles, kinetic energy can also arise from changes in electric potential energy. In this exercise, the alpha particle's kinetic energy comes from the work done by the electric field of the gold nucleus. When an alpha particle accelerates through an electric field created by a potential difference (voltage), its potential energy converts into kinetic energy.
This conversion allows the particle to reach closer distances to the gold nucleus, overcoming the natural repulsive forces between positively charged entities.
Ultimately, the amount of kinetic energy gained by the particle is dictated by the potential difference applied, thus influencing how close it can approach another charged body like a gold nucleus.

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Most popular questions from this chapter

A metal sphere with radius \(r_a\) is supported on an insulating stand at the center of a hollow, metal, spherical shell with radius \(r_b\) . There is charge \(+\)q on the inner sphere and charge \(-\)q on the outer spherical shell. (a) Calculate the potential \(V(r)\) for (i) \(r < r_a ;\) (ii) \(r_a < r < r_b ;\) (iii) \(r > r_b .\) (\(Hint\): The net potential is the sum of the potentials due to the individual spheres.) Take \(V\) to be zero when \(r\) is infinite. (b) Show that the potential of the inner sphere with respect to the outer is $$V_{ab} = \frac{q} {4\pi\epsilon_0} ( \frac{1} {r_a} - \frac{1} {r_b} )$$ (c) Use Eq. (23.23) and the result from part (a) to show that the electric field at any point between the spheres has magnitude $$E(r) = \frac {V_{ab}} {(1/r_a - 1/r_b)}\frac {1} {r_2}$$ (d) Use Eq. (23.23) and the result from part (a) to find the electric field at a point outside the larger sphere at a distance \(r\) from the center, where \(r > r_b\) . (e) Suppose the charge on the outer sphere is not \(-q\) but a negative charge of different magnitude, say \(-Q\). Show that the answers for parts (b) and (c) are the same as before but the answer for part (d) is different.

A charge of 28.0 nC is placed in a uniform electric field that is directed vertically upward and has a magnitude of 4.00 \(\times 10^4\) V\(/\)m. What work is done by the electric force when the charge moves (a) 0.450 m to the right; (b) 0.670 m upward; (c) 2.60 m at an angle of 45.0\(^\circ\) downward from the horizontal?

When radium-226 decays radioactively, it emits an alpha particle (the nucleus of helium), and the end product is radon-222. We can model this decay by thinking of the radium-226 as consisting of an alpha particle emitted from the surface of the spherically symmetric radon-222 nucleus, and we can treat the alpha particle as a point charge. The energy of the alpha particle has been measured in the laboratory and has been found to be 4.79 MeV when the alpha particle is essentially infinitely far from the nucleus. Since radon is much heavier than the alpha particle, we can assume that there is no appreciable recoil of the radon after the decay. The radon nucleus contains 86 protons, while the alpha particle has 2 protons and the radium nucleus has 88 protons. (a) What was the electric potential energy of the alpha\(-\)radon combination just before the decay, in MeV and in joules? (b) Use your result from part (a) to calculate the radius of the radon nucleus.

A particle with charge \(+\)7.60 nC is in a uniform electric field directed to the left. Another force, in addition to the electric force, acts on the particle so that when it is released from rest, it moves to the right. After it has moved 8.00 cm, the additional force has done 6.50 \(\times 10^{-5}\) J of work and the particle has 4.35 \(\times 10^{-5}\) J of kinetic energy. (a) What work was done by the electric force? (b) What is the potential of the starting point with respect to the end point? (c) What is the magnitude of the electric field?

Two point charges of equal magnitude \(Q\) are held a distance \(d\) apart. Consider only points on the line passing through both charges. (a) If the two charges have the same sign, find the location of all points (if there are any) at which (i) the potential (relative to infinity) is zero (is the electric field zero at these points?), and (ii) the electric field is zero (is the potential zero at these points?). (b) Repeat part (a) for two point charges having opposite signs.

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