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(I) What potential difference is needed to give a helium nucleus \((Q = 2e)\) 85.0 keV of kinetic energy?

Short Answer

Expert verified
The potential difference required is approximately 42,500 V.

Step by step solution

01

Understanding the Problem

We need to find the potential difference needed to give a helium nucleus with charge \(Q = 2e\) a kinetic energy of 85.0 keV. The potential difference \(V\) is related to the change in kinetic energy \(E_k\) of the charge \(Q\) by the formula \( E_k = QV \).
02

Convert Kinetic Energy to Joules

The kinetic energy provided is 85.0 keV. To use it in further calculations, we need to convert it into joules. Knowing that 1 electronvolt (eV) is equal to \(1.602 \times 10^{-19}\) joules, we have:\[ E_k = 85.0 \times 10^3 \times 1.602 \times 10^{-19} = 1.3617 \times 10^{-14} \text{ J} \]
03

Determine Charge of Helium Nucleus

The helium nucleus carries a charge of \(Q = 2e\), where \(e\) is the elementary charge \(1.602 \times 10^{-19} \text{ C}\). So the total charge is:\[ Q = 2 \times 1.602 \times 10^{-19} = 3.204 \times 10^{-19} \text{ C} \]
04

Apply Formula to Find Potential Difference

Using the formula \( E_k = QV \), where \(E_k = 1.3617 \times 10^{-14} \text{ J}\) and \(Q = 3.204 \times 10^{-19} \text{ C}\), solve for the potential difference \(V\):\[ V = \frac{E_k}{Q} = \frac{1.3617 \times 10^{-14}}{3.204 \times 10^{-19}} \text{ V} \]Calculating this, we find:\[ V \approx 4.25 \times 10^4 \text{ V} = 42,500 \text{ V} \]
05

Result Interpretation

The potential difference required to give a helium nucleus a kinetic energy of 85.0 keV is approximately 42,500 volts. This means that if the helium nucleus crosses this potential difference, it would gain the given kinetic energy.

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Key Concepts

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

Potential Difference
A potential difference, also known as voltage, is a measure of the work needed to move a charge from one point to another in an electric field. It is denoted by the symbol \(V\) and typically measured in volts (V). In the context of this exercise, we must calculate the potential difference required to impart a specific kinetic energy to a helium nucleus.

The relationship between potential difference and kinetic energy in this scenario is given by the formula:
  • \( E_k = QV \)
where \(E_k\) is the kinetic energy, \(Q\) is the charge of the helium nucleus, and \(V\) is the potential difference. Thus, the potential difference is crucial in this energy transfer because it determines how much kinetic energy can be gained by the helium nucleus as it traverses through the electric field.

By calculating the potential difference, we are effectively assessing how much energy per unit charge is available to be transferred to the charged particle, altering its kinetic state.
Kinetic Energy
Kinetic energy is the energy of motion. It can be understood as the energy required to accelerate an object from the rest to its current velocity. In our exercise, the helium nucleus is accelerated to achieve a kinetic energy of 85.0 keV (kiloelectronvolts).

In physical contexts:
  • \(1 \text{ eV} = 1.602 \times 10^{-19} \text{ joules}\)
Converting kinetic energy from keV to joules makes it easier to work in standard SI units in calculations. In this problem, converting 85.0 keV to joules results in \(1.3617 \times 10^{-14} \text{ J}\).

Understanding kinetic energy allows us to see how potential differences contribute to altering the velocity and movement energy of particles such as the helium nucleus within electric fields.
Helium Nucleus
A helium nucleus, also known as an alpha particle, consists of two protons and two neutrons. This structure gives it a specific set of properties, particularly in electrostatic interactions.

The charge of a helium nucleus is significant in numerical terms:
  • \(Q = 2e = 3.204 \times 10^{-19} \text{ C}\)
where \(e\) is the elementary charge, approximately \(1.602 \times 10^{-19} \text{ C}\). The significance of the helium nucleus's charge lies in how it influences the dynamics as it moves within an electric field. The total charge impacts the force experienced by the particle due to electric potentials and thus affects the kinetic energy gained or lost during motion.
Conservation of Energy
The conservation of energy is a fundamental principle in physics stating that energy cannot be created or destroyed, only transformed from one form to another. In the context of this exercise involving a helium nucleus, this principle helps us understand why and how kinetic energy changes as it moves across a potential difference.

When dealing with charged particles:
  • The sum of kinetic energy and potential energy remains constant.
This principle ensures that any decrease in the potential energy of the nucleus is directly associated with an increase in its kinetic energy, as described by the equation \(E_k = QV\).

Therefore, conservation of energy is invaluable for predicting the outcomes of energy transformations within electrostatic systems and ensures that the calculated potential difference correctly reflects the energy dynamics described in the original exercise.

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Most popular questions from this chapter

In the \(\textbf{dynamic random access memory (DRAM)}\) of a computer, each memory cell contains a capacitor for charge storage. Each of these cells represents a single binarybit value of "1" when its 35-fF capacitor (1 fF = 10\(^{-15}\)) is charged at 1.5 V, or "0" when uncharged at 0 V. (a) When fully charged, how many excess electrons are on a cell capacitor's negative plate? (\(b\)) After charge has been placed on a cell capacitor's plate, it slowly "leaks" off at a rate of about 0.30fC/s. How long does it take for the potential difference across this capacitor to decrease by 2.0\(\%\) from its fully charged value? (Because of this leakage effect, the charge on a DRAM capacitor is "refreshed" many times per second.) Note: A DRAM cell is shown in Fig. 21-29.

(II) The electric field between the plates of a paper-separated (\(K =\) 3.75) capacitor is 8.24 \(\times\) 10\(^4\)V/m. The plates are 1.95 mm apart, and the charge on each is 0.675 \(\mu\)C. Determine the capacitance of this capacitor and the area of each plate.

In an older television tube, electrons are accelerated by thousands of volts through a vacuum. If a television set were laid on its back, would electrons be able to move upward against the force of gravity? What potential difference, acting over a distance of 2.4 cm, would be needed to balance the downward force of gravity so that an electron would remain stationary? Assume that the electric field is uniform.

A parallel-plate capacitor with plate area \(A =\) 2.0 m\(^2\) and plate separation \(d =\) 3.0 mm is connected to a 35-V battery (Fig. 17-51a). (\(a\)) Determine the charge on the capacitor, the electric field, the capacitance, and the energy stored in the capacitor. (\(b\)) With the capacitor still connected to the battery, a slab of plastic with dielectric strength \(K =\) 3.2 is placed between the plates of the capacitor, so that the gap is completely filled with the dielectric (Fig. 17-51b).What are the new values of charge, electric field, capacitance, and the energy stored in the capacitor?

Compact "ultracapacitors" with capacitance values up to several thousand farads are now commercially available. One application for ultracapacitors is in providing power for electrical circuits when other sources (such as a battery) are turned off. To get an idea of how much charge can be stored in such a component, assume a 1200-F ultracapacitor is initially charged to 12.0 V by a battery and is then disconnected from the battery. If charge is then drawn off the plates of this capacitor at a rate of 1.0mC/s, say, to power the backup memory of some electrical device, how long (in days) will it take for the potential difference across this capacitor to drop to 6.0 V?

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