Effect of frequency of incident radiation on stopping potential - 11.4.3 | 11. DUAL NATURE OF RADIATION AND MATTER | CBSE 12 Physics Part 2
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Introduction to Stopping Potential

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0:00
Teacher
Teacher

Today, we're going to explore stopping potential in the context of the photoelectric effect. Can anyone explain what we mean by 'stopping potential'?

Student 1
Student 1

Is it the minimum voltage needed to stop electrons from reaching the collector plate?

Teacher
Teacher

Exactly, well done! The stopping potential is indeed the critical value that opposes the motion of the most energetic photoelectrons. Now, can anyone tell me how this relates to the frequency of the light used?

Student 2
Student 2

I think it changes based on the frequency. Higher frequencies mean more energy.

Teacher
Teacher

That's correct! The kinetic energy of the ejected electrons increases with the frequency of incident light, thereby requiring a higher stopping potential to halt these electrons. Remember this key point: 'Frequency Up, Stopping Potential Up!'

Linear Relationship Between Frequency and Stopping Potential

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0:00
Teacher
Teacher

Okay, now let’s discuss the relationship between frequency and stopping potential. Who can summarize this relationship for me?

Student 3
Student 3

The stopping potential increases linearly with frequency, right?

Teacher
Teacher

Absolutely! This linearity means that as you increase the frequency of the incident light, the stopping potential needed to halt the electrons also increases. If we plot this, we get a straight line. How does this compare to the effect of intensity?

Student 4
Student 4

Intensity doesn’t change the stopping potential; it only affects the number of electrons emitted, not their energy.

Teacher
Teacher

Exactly! So, remember: 'Intensity affects quantity, frequency affects quality!' Great job!

Threshold Frequency

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0:00
Teacher
Teacher

Let’s now shift our focus to the concept of threshold frequency. Who can explain what this means?

Student 1
Student 1

It’s the minimum frequency needed for photoelectric emission to occur, right?

Teacher
Teacher

Exactly! If the frequency of light is lower than this threshold frequency, no photoelectrons will be emitted regardless of how intense the light is. How would you find the threshold frequency for different materials?

Student 2
Student 2

We would need to look at the work function for those materials, then use the equation to find it.

Teacher
Teacher

Great point! Always connect the stopping potential to the threshold frequency via the work function. Keep in mind: 'Threshold Frequency = Key for Emission!'

Kinetic Energy of Photoelectrons

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0:00
Teacher
Teacher

Now that we know about stopping potential and threshold frequency, how do these concepts inform us about the kinetic energy of photoelectrons?

Student 3
Student 3

The kinetic energy should increase with frequency, right? It’s related to the stopping potential.

Teacher
Teacher

Correct! The maximum kinetic energy of emitted photoelectrons increases as the frequency increases, and it is given as K_max = eV₀. This means the stopping potential directly represents the energy needed to stop these electrons.

Student 4
Student 4

So, higher frequency not only increases stopping potential but also maximum kinetic energy?

Teacher
Teacher

Exactly! Summarizing: 'More Frequency = More Energy!' Remember, this is a critical concept in understanding the photoelectric effect.

Introduction & Overview

Read a summary of the section's main ideas. Choose from Basic, Medium, or Detailed.

Quick Overview

This section discusses how the frequency of incident radiation affects the stopping potential in the photoelectric effect.

Standard

The section explains that as the frequency of the incident radiation increases, the stopping potential also increases, indicating that the maximum kinetic energy of emitted electrons is directly related to the frequency of the radiation rather than its intensity.

Detailed

In this section, we explore the relationship between the frequency of incident radiation and the stopping potential (V₀) necessary to halt photoelectric emission from a metal surface. It is established that the energy of emitted electrons is dependent on the frequency of radiation, with higher frequencies resulting in higher stopping potentials. Detailed observations indicate that the stopping potential varies linearly with frequency, while remaining independent of intensity. This leads to the conclusion that the maximum kinetic energy of photoelectrons correlates directly with frequency, as given by the formula K_max = eV₀, which conforms to the findings of the photoelectric effect. Furthermore, a threshold frequency exists for each material, below which no electrons can be emitted, regardless of the intensity of incident light.

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Audio Book

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Variation of Stopping Potential with Frequency

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We now study the relation between the frequency n of the incident radiation and the stopping potential V₀. We suitably adjust the same intensity of light radiation at various frequencies and study the variation of photocurrent with collector plate potential. The resulting variation is shown in Fig. 11.4. We obtain different values of stopping potential but the same value of the saturation current for incident radiation of different frequencies. The energy of the emitted electrons depends on the frequency of the incident radiations. The stopping potential is more negative for higher frequencies of incident radiation.

Detailed Explanation

This chunk explains how the stopping potential (V₀) of photoelectrons varies with the frequency (n) of the incident radiation. As the frequency increases, the energy that electrons gain also increases, and higher stopping potentials are needed to prevent these more energetic electrons from reaching the collector plate. This means that if we shine light at different frequencies but with the same intensity, we will get different stopping potentials.

Examples & Analogies

Imagine a game where you are kicking balls at a target—it’s easier to stop a slow ball than a faster one. Similarly, the photoelectrons ejected by light at a higher frequency have more energy (like the fast balls), and therefore, require a stronger opposing force (higher stopping potential) to stop them.

Linear Relationship Between Frequency and Stopping Potential

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Note from Fig. 11.4 that the stopping potentials are in the order V₀₃ > V₀₂ > V₀₁ if the frequencies are in the order n₃ > n₂ > n₁. This implies that greater the frequency of incident light, greater is the maximum kinetic energy of the photoelectrons. Consequently, we need greater retarding potential to stop them completely. If we plot a graph between the frequency of incident radiation and the corresponding stopping potential for different metals we get a straight line.

Detailed Explanation

The stopping potential not only increases with frequency, but this increase is linear. This means that if you were to graph these two variables, you'd get a straight line, indicating a direct relationship. The greater the frequency of the incoming light, the more energy the electrons have, thus requiring a higher stopping potential to prevent them from passing through.

Examples & Analogies

Think of it like the amount of force needed to stop a car. If the car is going faster (higher frequency), more force (higher stopping potential) is required to halt its movement. The straight line on a graph represents the consistent relationship between the speed of the car (frequency) and the power required to stop it.

Threshold Frequency and Photoelectric Emission

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These observations have two implications: (i) The maximum kinetic energy of the photoelectrons varies linearly with the frequency of incident radiation, but is independent of its intensity. (ii) For a frequency n₀ of incident radiation, lower than the cut-off frequency n₀, no photoelectric emission is possible even if the intensity is large. This minimum, cut-off frequency n₀ is called the threshold frequency. It is different for different metals.

Detailed Explanation

The threshold frequency is critical because it is the minimum frequency needed for photoelectric emission to occur. Below this frequency, no matter how much light is shining on the metal, electrons will not be ejected. This establishes two important points: the kinetic energy of the emitted electrons is related to the frequency of the light, and there is a limit (the threshold frequency) below which no emission occurs regardless of light intensity.

Examples & Analogies

Consider a door that only opens if you push with enough force. The threshold frequency is like the minimum push needed to make the door swing open. If you don’t push hard enough (lower frequency), it stays shut (no electron emission), regardless of how much you press (light intensity).

Instantaneous Photoelectric Emission

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Note that in all the above experiments, it is found that, if frequency of the incident radiation exceeds the threshold frequency, the photoelectric emission starts instantaneously without any apparent time lag, even if the incident radiation is very dim.

Detailed Explanation

This chunk addresses how quickly photoelectrons are emitted once the incident light frequency surpasses the threshold frequency. It emphasizes that the emission is almost instantaneous, signifying that this process occurs swiftly as the electrons absorb energy from the photons in the light.

Examples & Analogies

Imagine a light switch that turns on instantly when you flip it. The moment you flip the switch (reach the threshold), the light comes on (electrons are emitted) without delay. This highlights how light can have immediate effects upon interacting with the right materials.

Definitions & Key Concepts

Learn essential terms and foundational ideas that form the basis of the topic.

Key Concepts

  • Stopping Potential: The voltage needed to stop the most energetic photoelectrons.

  • Threshold Frequency: The minimum frequency required for photoelectric emission.

  • Kinetic Energy of Photoelectrons: The energy of emitted electrons relates directly to the frequency, not intensity.

  • Linearity of Stopping Potential and Frequency: Stopping potential increases linearly with increasing frequency.

Examples & Real-Life Applications

See how the concepts apply in real-world scenarios to understand their practical implications.

Examples

  • Consider a metal with a threshold frequency of 5 x 10^14 Hz. If light with a frequency of 7 x 10^14 Hz is applied, photoemission occurs, and the stopping potential can be calculated.

  • Using a stopping potential of 1.2 V for a frequency of incident radiation of 6 x 10^14 Hz, we can determine the maximum kinetic energy of electrons ejected.

Memory Aids

Use mnemonics, acronyms, or visual cues to help remember key information more easily.

🎵 Rhymes Time

  • For emission in the light so bright, frequency is key, keeping electrons in flight.

📖 Fascinating Stories

  • Imagine a race: the higher the frequency of the light, the faster the electrons can run away. But if the light doesn't meet the threshold, they’re stuck, unable to leave.

🧠 Other Memory Gems

  • F-S-K: Frequency increases Stopping potential and Kinetic energy.

🎯 Super Acronyms

SFT

  • Stopping Potential
  • Frequency
  • Threshold - remember these for photoelectric effect.

Flash Cards

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Glossary of Terms

Review the Definitions for terms.

  • Term: Stopping Potential (V₀)

    Definition:

    The minimum potential needed to stop the most energetic photoelectrons from reaching the collector plate.

  • Term: Threshold Frequency (n₀)

    Definition:

    The minimum frequency of incident light required to emit photoelectrons from a material.

  • Term: Kinetic Energy (K_max)

    Definition:

    The maximum energy of emitted photoelectrons, which is determined by the frequency of the incident radiation.

  • Term: Photoelectric Effect

    Definition:

    The emission of electrons from a material when it is illuminated by light of sufficient frequency.

  • Term: Work Function (f₀)

    Definition:

    The minimum energy needed for an electron to escape from the surface of a metal.