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Which of the following angles between an electric dipole moment and an applied electric field will result in the most stable state? a) \(0 \mathrm{rad}\) d) The electric dipole moment is b) \(\pi / 2\) rad not stable under any condition in c) \(\pi\) rad an applied electric field.

Short Answer

Expert verified
Answer: a) \(0 \mathrm{rad}\)

Step by step solution

01

Understand the electric dipole moment and potential energy

In a system with an electric dipole moment and an applied electric field, the potential energy (U) of the system can be described as: $$ U = -\vec{p} \cdot \vec{E} $$ where \(\vec{p}\) is the electric dipole moment and \(\vec{E}\) is the applied electric field. The dot product between the two vectors depends on the angle between them, denoted as \(\theta\). Therefore, the potential energy formula can be rewritten as: $$ U = -p E \cos{\theta} $$
02

Analyze the potential energy with respect to the angle θ

We need to determine which angle θ between the electric dipole moment and applied electric field results in the most stable state. The most stable state corresponds to the lowest potential energy. We can examine the given options one by one. Let's evaluate the potential energy for each given angle: 1. Angle θ = \(0 \mathrm{rad}\): $$ U_{0} = -p E \cos{(0 \mathrm{rad})} = -p E $$ 2. Angle θ = \(\pi / 2\) rad: $$ U_{\pi/2} = -p E \cos{(\pi / 2 \mathrm{rad})} = 0 $$ 3. Angle θ = \(\pi\) rad: $$ U_{\pi} = -p E \cos{(\pi \mathrm{rad})} = p E $$
03

Determine the angle corresponding to the most stable state

To find the most stable state, we need to find the angle that results in the lowest potential energy. Comparing the values of the potential energy calculated in step 2, we can see that: - \(U_{0}\) = \(-p E\): The potential energy is negative, indicating a stable state. - \(U_{\pi/2}\) = \(0\): The potential energy is equal to zero, indicating a less stable state than when the potential energy is negative. - \(U_{\pi}\) = \(p E\): The potential energy is positive, indicating an unstable state. Therefore, the angle that results in the most stable state is \(0 \mathrm{rad}\), as it leads to the lowest potential energy. Hence, the correct answer is: a) \(0 \mathrm{rad}\)

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Key Concepts

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

Understanding Potential Energy in Electric Fields
Potential energy is a key concept in physics, especially when discussing electric dipoles within an electric field. An electric dipole consists of two opposite charges separated by a distance. The potential energy, denoted as \( U \), in the presence of an applied electric field \( \vec{E} \), can be defined as:\[ U = -\vec{p} \cdot \vec{E} \]where \( \vec{p} \) is the electric dipole moment.

The formula simplifies to:\[ U = - p E \cos{\theta} \]\( \theta \) is the angle between the dipole moment and the electric field vector.
  • When \( \theta = 0 \), \( \cos{\theta} = 1 \), resulting in \( U = -pE \), the lowest potential energy, indicating highest stability.
  • When \( \theta = \pi/2 \), \( \cos{\theta} = 0 \), resulting in \( U = 0 \), meaning less stability compared to when the potential energy is negative.
  • When \( \theta = \pi \), \( \cos{\theta} = -1 \), leading to \( U = pE \), which is the highest potential energy, indicative of an unstable state.
These principles help in determining the stability of an electric dipole in an applied field.
Role of Applied Electric Field
An applied electric field influences the orientation and behavior of electric dipoles. The external field initiates forces on the dipole, causing it to align itself in the direction of the field.

The electric field \( \vec{E} \) interacts with the dipole moment \( \vec{p} \), producing a torque that tends to rotate the dipole to minimize potential energy.
  • At \( \theta = 0 \), the dipole is aligned with the field, maximizing the effectiveness of this alignment.
  • At \( \theta = \pi/2 \), the dipole is perpendicular to the field, minimizing interaction.
  • At \( \theta = \pi \), the dipole is opposite to the field, leading to maximum potential energy and instability.
Understanding how an electric field acts on a dipole helps predict and control system behaviors, crucial in fields like chemistry and electronics.
Stability in Electric Fields
Stability in electric fields is all about the orientation of the electric dipole relative to the field. A stable configuration minimizes potential energy, resulting in less movement or disturbance in the system.

For an electric dipole in a field:
  • Stable State (\( \theta = 0 \)): The dipole aligns with the field, meaning less potential for rotational motion and energy loss. This alignment maintains the system's equilibrium.
  • Neutral State (\( \theta = \pi/2 \)): The dipole is perpendicular. Here, the forces are balanced, but it's neither fully stable nor unstable.
  • Unstable State (\( \theta = \pi \)): The dipole opposes the field direction, attempting to realign when disturbed since any external force can cause movement.
The concept of stability is vital in applications like molecular interactions and designing stable electric components, where unwanted motion can disrupt performance.

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Most popular questions from this chapter

Using Gauss's Law and the relation between electric potential and electric field, show that the potential outside a uniformly charged sphere is identical to the potential of a point charge placed at the center of the sphere and equal to the total charge of the sphere. What is the potential at the surface of the sphere? How does the potential change if the charge distribution is not uniform but has spherical (radial) symmetry?

Nuclear fusion reactions require that positively charged nuclei be brought into close proximity, against the electrostatic repulsion. As a simple example, suppose a proton is fired at a second, stationary proton from a large distance away. What kinetic energy must be given to the moving proton to get it to come within \(1.00 \cdot 10^{-15} \mathrm{~m}\) of the target? Assume that there is a head-on collision and that the target is fixed in place.

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

A thin line of charge is aligned along the positive \(y\) -axis from \(0 \leq y \leq L,\) with \(L=4.0 \mathrm{~cm} .\) The charge is not uniformly distributed but has a charge per unit length of \(\lambda=A y,\) with \(A=\) \(8.0 \cdot 10^{-7} \mathrm{C} / \mathrm{m}^{2}\). Assuming that the electric potential is zero at infinite distance, find the electric potential at a point on the \(x\) -axis as a function of \(x\). Give the value of the electric potential at \(x=3.0 \mathrm{~cm} .\)

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