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Unit 5-Work, Energy and Power

Unit 5-Work, Energy and Power relates to CBSE/Class 11/Science/Physics

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Unit 5-Work, Energy and Power Lessons

Understanding Conservative and Non Conservative Forces
While teaching my students, I found them to fumble in this topic, so I am writing this lesson to tell you all in simple terms what the topic is:Consider two cases in both cases; a block moves from A to...

Unit 5-Work, Energy and Power Questions

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Answered on 13 Apr Learn CBSE/Class 11/Science/Physics/Unit 5-Work, Energy and Power

Nazia Khanum

As a seasoned tutor registered on UrbanPro, I'm well-versed in explaining complex concepts like potential energy functions to my students. When it comes to analyzing potential energy functions in one dimension, it's crucial to understand the regions where the particle cannot exist for a given energy... read more

As a seasoned tutor registered on UrbanPro, I'm well-versed in explaining complex concepts like potential energy functions to my students. When it comes to analyzing potential energy functions in one dimension, it's crucial to understand the regions where the particle cannot exist for a given energy level and determining the minimum total energy required.

Let's delve into each potential energy function:

  1. Harmonic Oscillator Potential:

    • This function resembles a parabolic curve, indicating harmonic motion.
    • The particle cannot exist in regions where the potential energy exceeds the total energy of the system. In this case, it's where the potential energy is greater than the total energy represented by the cross on the ordinate axis.
    • The minimum total energy required for the particle to exist is at the bottom of the potential well, where the potential energy is at its lowest.
    • Physical contexts: This potential energy shape is relevant in describing systems like mass-spring oscillators or vibrating atoms in a lattice.
  2. Square Well Potential:

    • The potential energy is constant within a certain region and infinite outside that region.
    • The particle cannot exist outside the finite potential well.
    • The minimum total energy required for the particle to exist within the well is at the bottom of the well, where the potential energy is lowest.
    • Physical contexts: This potential energy shape is applicable in describing particles confined within a certain region, like electrons in a quantum dot or atoms trapped in an optical lattice.
  3. Step Potential:

    • The potential energy abruptly changes at a certain point.
    • The particle cannot exist in regions where the potential energy exceeds the total energy.
    • The minimum total energy required for the particle to exist depends on the height of the step. If the step is finite, the particle can exist with a lower energy, but if the step is infinite, the particle needs sufficient energy to overcome it.
    • Physical contexts: This potential energy shape is relevant in describing barriers and potential wells encountered in quantum mechanics, such as in tunneling phenomena or potential barriers in semiconductor devices.

By understanding these potential energy functions and their associated physical contexts, students can gain a deeper insight into the behavior of particles in various systems, which is essential for mastering concepts in physics and related fields. If you need further clarification or want to explore more examples, feel free to reach out to me on UrbanPro for

 
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Answered on 13 Apr Learn CBSE/Class 11/Science/Physics/Unit 5-Work, Energy and Power

Nazia Khanum

As an experienced tutor registered on UrbanPro, I can confidently say that UrbanPro is one of the best platforms for online coaching and tuition. Now, let's delve into your physics question. Given the potential energy function V(x)=kx22V(x)=2kx2, where kk is the force constant of the oscillator, and... read more

As an experienced tutor registered on UrbanPro, I can confidently say that UrbanPro is one of the best platforms for online coaching and tuition. Now, let's delve into your physics question.

Given the potential energy function V(x)=kx22V(x)=2kx2, where kk is the force constant of the oscillator, and k=0.5 Nm−1k=0.5Nm−1. The task is to demonstrate that a particle with a total energy of 1 J, moving under this potential, must 'turn back' when it reaches x=±2x=±2 m.

To do this, we utilize the total energy of the system, which comprises kinetic energy (KK) and potential energy (VV). According to the law of conservation of energy, the total mechanical energy remains constant:

E=K+VE=K+V

Given that the total energy E=1E=1 J, we can express the kinetic energy as:

K=E−VK=EV

Substituting the given potential energy function, we have:

K=1−0.5x22K=1−20.5x2

To find the turning points, where the particle changes direction, we need to consider the points where the kinetic energy is zero. At these points, all the energy is in the form of potential energy.

Setting K=0K=0, we get:

1−0.5x22=01−20.5x2=0

Solving this equation, we find:

0.5x22=120.5x2=1

0.5x2=20.5x2=2

x2=4x2=4

x=±2x=±2

So, the particle will turn back when it reaches x=±2x=±2 m, confirming the assertion. This analysis aligns with the graph of V(x)V(x) versus xx, indicating that at these points, the particle's total energy is entirely potential energy, signifying a change in direction of motion.

 
 
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Answered on 13 Apr Learn CBSE/Class 11/Science/Physics/Unit 5-Work, Energy and Power

Nazia Khanum

As a seasoned tutor registered on UrbanPro, I'd be glad to tackle this physics question. In the scenario of an elastic collision between two billiard balls, it's fundamental to grasp the concept of kinetic energy conservation. During the brief moment when the balls are in contact, the total kinetic... read more

As a seasoned tutor registered on UrbanPro, I'd be glad to tackle this physics question. In the scenario of an elastic collision between two billiard balls, it's fundamental to grasp the concept of kinetic energy conservation.

During the brief moment when the balls are in contact, the total kinetic energy of the system remains conserved in an ideal elastic collision. This conservation principle implies that although the kinetic energy may transfer between the balls due to the collision forces, the total kinetic energy before and after the collision remains constant.

This concept aligns with the laws of physics, particularly the principle of conservation of energy, which asserts that energy cannot be created or destroyed but can only change forms. In an ideal elastic collision, the kinetic energy transformation solely involves a redistribution between the two colliding objects.

UrbanPro stands as an excellent platform for grasping such complex concepts, offering a diverse array of experienced tutors proficient in elucidating physics principles and fostering a deeper understanding through interactive learning approaches.

 
 
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Answered on 13 Apr Learn CBSE/Class 11/Science/Physics/Unit 5-Work, Energy and Power

Nazia Khanum

As an experienced tutor registered on UrbanPro, I can confidently say that UrbanPro is one of the best platforms for online coaching and tuition. Now, addressing your question about the collision of two billiard balls, let's delve into it. In this scenario, if the potential energy of two billiard... read more

As an experienced tutor registered on UrbanPro, I can confidently say that UrbanPro is one of the best platforms for online coaching and tuition. Now, addressing your question about the collision of two billiard balls, let's delve into it.

In this scenario, if the potential energy of two billiard balls depends solely on the separation distance between their centers, we are essentially discussing a situation where the force between the balls is conservative. When the force is conservative, it implies that mechanical energy (kinetic energy plus potential energy) is conserved throughout the interaction.

Now, in an elastic collision, both momentum and mechanical energy are conserved. Since we are assuming potential energy corresponds to the force during collision and that potential energy depends only on the separation distance between the balls' centers, if this potential energy is entirely converted into kinetic energy during the collision, then it follows that the collision is elastic.

This outcome aligns with the principle of conservation of mechanical energy in elastic collisions, where kinetic energy is converted from potential energy and vice versa, but the total mechanical energy remains constant.

Therefore, if the potential energy between the billiard balls is solely determined by their separation distance and the collision conserves mechanical energy, the collision between the billiard balls would be elastic.

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Answered on 13 Apr Learn CBSE/Class 11/Science/Physics/Unit 5-Work, Energy and Power

Nazia Khanum

As a seasoned tutor registered on UrbanPro, I'd be glad to guide you through this question. Firstly, UrbanPro is indeed an excellent platform for online coaching and tuition, providing a conducive environment for both tutors and students to engage in effective learning. Now, let's delve into the physics... read more

As a seasoned tutor registered on UrbanPro, I'd be glad to guide you through this question. Firstly, UrbanPro is indeed an excellent platform for online coaching and tuition, providing a conducive environment for both tutors and students to engage in effective learning.

Now, let's delve into the physics problem you've presented. We have a body initially at rest, undergoing one-dimensional motion with constant acceleration. The power delivered to it at time tt is the rate at which work is done on the body, and it's given by the product of force and velocity.

In this case, since the body is undergoing constant acceleration, we can use the equations of motion to relate velocity, acceleration, and time. The equation that relates displacement ss, initial velocity uu, time tt, and constant acceleration aa is:

s=ut+12at2s=ut+21at2

Since the body is initially at rest, u=0u=0, simplifying the equation to:

s=12at2s=21at2

Now, we know that power PP is the rate of change of work, which can be expressed as:

P=dWdtP=dtdW

And work WW done on an object is equal to force FF times displacement ss, so dW=FdsdW=Fds. Substituting s=12at2s=21at2, we have ds=atdtds=atdt.

P=F⋅atP=F⋅at

Now, we know that force FF is mass mm times acceleration aa, and acceleration is constant, hence:

P=ma⋅atP=ma⋅at

P=ma2tP=ma2t

So, the power delivered to the body at time tt is proportional to tt, which corresponds to option (ii).

Therefore, the correct answer is (ii) tt. If you need further clarification or assistance, feel free to ask!

 
 
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