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Wave mechanical model of the atom depends upon (1) de Broglie concept of dual nature of electron (2) Heisenberg uncertainty principle (3) Schrodinger wave equation (4) All the above

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All the above.

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01

- Understand de Broglie's Concept

de Broglie's concept introduced the idea that particles such as electrons exhibit both particle and wave properties. This is known as the dual nature of the electron, which is fundamental to the wave mechanical model of the atom.
02

- Review Heisenberg Uncertainty Principle

Heisenberg's uncertainty principle states that it is impossible to simultaneously know both the exact position and exact momentum of an electron. This principle is crucial for the wave mechanical model as it implies a probabilistic approach to describing electron locations.
03

- Examine Schrodinger Wave Equation

Schrodinger wave equation is a key mathematical model that describes how the quantum state of a physical system changes with time. It incorporates the wave-like behavior of electrons and is integral to the wave mechanical model of the atom.
04

- Conclusion

By understanding all three components - de Broglie's dual nature concept, Heisenberg's uncertainty principle, and Schrodinger's wave equation - it is clear that the wave mechanical model depends on all these principles collectively.

Key Concepts

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

de Broglie Dual Nature
In the early 20th century, the French physicist Louis de Broglie introduced a groundbreaking concept known as the 'dual nature' of matter. This idea suggests that particles, including electrons, can exhibit both particle-like and wave-like properties.
The de Broglie hypothesis posits that any moving particle or object has an associated wave. For electrons, this meant that they do not just behave as discrete particles but also have wave characteristics.
De Broglie formulated an equation to describe this duality, which is given by \[\text{λ = }\frac{h}{p}\]where λ is the wavelength associated with the particle, h is Planck's constant, and p is the momentum of the particle.
This concept was revolutionary as it bridged previously separate understandings of particles and waves, laying foundational groundwork for quantum mechanics. It is essential for explaining phenomena like electron diffraction, which supports the wave nature of electrons.
Heisenberg Uncertainty Principle
The Heisenberg Uncertainty Principle, formulated by Werner Heisenberg, is a fundamental concept in quantum mechanics. It states that it is impossible to simultaneously determine the exact position and exact momentum of a particle with absolute precision.
Mathematically, the principle can be expressed as:\[\text{Δx · Δp ≥ }\frac{h}{4π}\]where Δx represents the uncertainty in position, Δp represents the uncertainty in momentum, and h is Planck's constant.
This principle implies a fundamental limit to what can be known about a quantum system. Instead of deterministic paths, electrons are described in terms of probability distributions.
This insight is crucial for the wave mechanical model. It means that rather than picturing electrons as orbiting the nucleus in definite paths, we describe their probable locations with wave functions. This probabilistic approach leads to a more accurate description of atomic and subatomic systems.
Schrodinger Wave Equation
Erwin Schrodinger, an Austrian physicist, developed an equation that is central to the wave mechanical model of the atom. The Schrodinger Wave Equation describes how the quantum state of a physical system changes over time.
This equation incorporates the wave-like behavior of particles, such as electrons, and can be written as:\[\text{ĤΨ = EΨ}\]where Ĥ (the Hamiltonian operator) represents the total energy of the system, Ψ (the wave function) describes the probability amplitude of the particle's state, and E is the energy of the system.
The wave function Ψ provides information about the likelihood of finding an electron in a particular region around the nucleus. Solving the Schrodinger equation for an atom allows us to determine these probabilities and understand electron configurations.
This equation is integral to quantum mechanics and the wave mechanical model as it mathematically explains how electrons exist and behave in an atom. It is a powerful tool for predicting the behavior of electrons in different atomic and molecular structures, forming the basis for much of modern chemistry and physics.

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Most popular questions from this chapter

An electron that will have the highest energy in the set is (1) \(3,2,1, \frac{1}{2}\) (2) \(4,2,-1, \frac{1}{2}\) (3) \(4,1,0,-\frac{1}{2}\) (4) \(5,0,0, \frac{1}{2}\)

If the mass of the clectron is reduced to half, the Rydberg constant (1) Remains unchanged (2) Becomes half (3) Becomes double (4) Becomes one-fourth \(\left[\right.\) Hint \(\left.: R_{H}=\frac{2 \pi^{2} m e^{4}}{c h^{3}}\right]\)

Which of the following statement is correct? (1) The kinetic energy of photoclectrons increases lincarly with wavelength of the light. (2) Photoclectric effect can be explained based on corpuscular nature of light. (3) Einstein was awarded Nobel Prize in physies in 1921 for his theory of relativity. (4) The ratio of energy to frequency of electromagnetic radiation is called Rydberg's constant.

Which of the following statements is false? (1) For azimuthal quantum number \(l=3\), the maximum number of electrons will be 14 . (2) The concept of electron spin was introduced by Uhlenbeck and Goudsmit. (3) The principal quantum number of an atom represents size of the orbit and distance of electron from nucleus. (4) The shape of an orbital is governed by magnetic quantum number.

Among the following the correct statement(s) is/are (1) Increase in the frequency of the incident radiation increases the kinetic energy of photoelectrons. (2) Threshold wavelength depends upon work function. (3) The study of photoclectric effect is useful in understanding quantisation of energy. (4) To cross the threshold energy intensity of the light must be increased. (1) I, II and III (2) II, III and IV (3) I, III and IV (4) I, II, III and IV

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