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The first 25 years of the twentieth century were momentous for the rapid pace of change in scientists' understanding of the nature of matter. (a) How did Rutherford's experiments on the scattering of \(\alpha\) particles by a gold foil set the stage for Bohr's theory of the hydrogen atom? (b) In what ways is de Broglie's hypothesis, as it applies to electrons, consistent with J. J. Thomson's conclusion that the electron has mass? In what sense is it consistent with proposals preceding Thomson's work that the cathode rays are a wave phenomenon?

Short Answer

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(a) Rutherford's experiments on alpha-particle scattering led to the Rutherford atomic model, which consists of a small, dense, positively charged nucleus, surrounded by orbiting electrons. Bohr built upon this model by introducing the concept of quantization of electron orbits, which explained the observed discrete emission spectra of the hydrogen atom. (b) De Broglie's hypothesis, stating that the wavelength of a particle (\(\lambda\)) is inversely proportional to its momentum (\(p\)), is consistent with J.J. Thomson's conclusion that the electron has mass, as mass implies the existence of momentum, thus giving electrons wave-like properties. This also supports earlier proposals that cathode rays were a wave phenomenon, bridging the gap between particle and wave nature of electrons.

Step by step solution

01

Part (a) : Relation between Rutherford's experiments and Bohr's theory

Rutherford's experiments on alpha-particle scattering provided valuable insights into the structure of atoms, leading to the development of the Rutherford model. When alpha particles are fired at a thin gold foil, most of them pass straight through, while some are deflected by large angles. This observation led Rutherford to propose that the atom consists of a small and dense positively charged core called the nucleus, surrounded by electrons orbiting it. Bohr's theory of the hydrogen atom built upon Rutherford's model by introducing the concept of quantization of electron orbits. According to Bohr, electrons can only occupy certain discrete orbits around the nucleus and radiate or absorb energy when transitioning between these orbits. This quantization idea helped explain the observed discrete emission spectra of the hydrogen atom.
02

Part (b) : De Broglie's hypothesis and its consistency with electron's mass

De Broglie's hypothesis suggested that particles such as electrons could exhibit wave-like behavior. His hypothesis stated that the wavelength of a particle (\(\lambda\)) is inversely proportional to its momentum (\(p\)), given by the relation \(\lambda = \frac{h}{p}\), where \(h\) is the Planck constant. J.J. Thomson's conclusion that the electron has mass is consistent with de Broglie's hypothesis because having mass implies the existence of momentum. It means that an electron has a wavelength associated with it due to its mass and momentum, and thus it can exhibit wave-like properties.
03

Part (b) : De Broglie's hypothesis and its consistency with proposals on cathode rays

Prior to Thomson's discoveries, some scientists believed that cathode rays were a wave phenomenon. De Broglie's hypothesis supports this idea to some extent, as it implies that electrons can exhibit wave-like behavior due to their mass and momentum. In a sense, de Broglie's hypothesis bridges the gap between the particle and wave nature of electrons, providing a consistent and unifying framework to understand their behavior.

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Key Concepts

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

Rutherford's Gold Foil Experiment
Imagine firing a stream of tiny, positively charged alpha particles at an ultra-thin sheet of gold, much like tossing a handful of pebbles at a tree. If that tree were made of mostly empty space, you'd expect most pebbles to pass through unimpeded. This is precisely what happened in Rutherford's gold foil experiment, one of the groundbreaking tests in nuclear physics.

Rutherford observed that while the majority of alpha particles shot through the gold foil, a few deflected at astounding angles. These deflections couldn't be explained by the then-accepted 'plum pudding' model, which assumed that positive charge was evenly spread throughout the atom. Rutherford concluded that atoms must have a small, densely packed nucleus with considerable positive charge that repels the alpha particles. This nucleus is surrounded by much lighter, negatively charged electrons, orbiting much like planets around the sun. This model set the stage for Bohr's revolutionary ideas about atomic structure.

Understanding Rutherford's experiment helps us appreciate how scientists peeled back the layers of atomic mystery, dramatically changing our view from a homogenous blob of positive and negative charge to a highly structured miniature solar system.
Bohr's Theory of the Hydrogen Atom
Building on Rutherford's nucleus-centric model, Niels Bohr brought a new twist to atomic physics with his theory of the hydrogen atom. While Rutherford suggested electrons orbit the nucleus, Bohr proposed that they do so at only certain allowed distances, or 'energy levels'.

Why don't these orbiting electrons crash into the nucleus, spiraling to their doom? Bohr's model suggested that electrons can only gain or lose energy by leaping between fixed orbits in a quantum jump, never existing in-between. This explains why atoms emit light at specific wavelengths, resulting in a characteristic spectrum for each element. For hydrogen, the simplest atom with just one electron, these discrete spectral lines were a beautiful confirmation of Bohr's theory.

These ideas were bold and challenged the classical physics of the time, but they offered a tantalizingly simple explanation for complex spectral phenomena. Bohr's model was a pivotal moment in quantum theory, showing a tantalizing harmony between the behavior of atomic particles and the rules of quantum mechanics.
De Broglie's Hypothesis
Classical physics drew a clear line between particles, which have mass, and waves that carry energy through space. Enter Louis de Broglie, a French physicist with a daring proposition: particles could behave like waves and vice versa. De Broglie's hypothesis suggested that every moving particle, including electrons, embodies wave-like characteristics and thus has a wavelength associated with its momentum.

The equation \(\lambda = \frac{h}{p}\) binds together an object's wavelength (\(\lambda\)) with its momentum (\(p\)), bridged by Planck's constant (\(h\)), a fundamental quantity in quantum mechanics. This wave-particle duality reconciled Thomson's electron having mass hence momentum with earlier notions of electrons as wave phenomena. It suggested that while electrons are indeed particles with mass, as Thomson showed, they also produce interference patterns, a pure wave property, under the right conditions.

De Broglie's unifying approach led to the concept of wave-particle duality as a cornerstone of quantum mechanics, paving the way for the Heisenberg Uncertainty Principle and Schrödinger's wave equation. His insights deepened the understanding of foundational elements of particle physics, forever altering the way scientists viewed the microscopic realm.

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Most popular questions from this chapter

(a) Why does the Bohr model of the hydrogen atom violate the uncertainty principle? (b) In what way is the description of the electron using a wave function consistent with de Broglie's hypothesis? (c) What is meant by the term probability density? Given the wave function, how do we find the probability density at a certain point in space?

For orbitals that are symmetric but not spherical, the contour representations (as in Figures 6.22 and 6.23 ) suggest where nodal planes exist (that is, where the electron density is zero). For example, the \(p_{x}\) orbital has a node wherever \(x=0\). This equation is satisfied by all points on the \(y z\) plane, so this plane is called a nodal plane of the \(p_{x}\) orbital. (a) Determine the nodal plane of the \(p_{z}\) orbital. (b) What are the two nodal planes of the \(d_{x y}\) orbital? (c) What are the two nodal planes of the \(d_{x^{2}-y^{2}}\) orbital?

Sketch the shape and orientation of the following types of orbitals: \((\mathbf{a}) s,(\mathbf{b}) p_{z},(\mathbf{c}) d_{x y}\)

Neutron diffraction is an important technique for determining the structures of molecules. Calculate the velocity of a neutron needed to achieve a wavelength of \(0.955 \AA .\) (Refer to the inside cover for the mass of the neutron).

The visible emission lines observed by Balmer all involved \(n_{f}=2 .\) (a) Explain why only the lines with \(n_{f}=2\) were observed in the visible region of the electromagnetic spectrum. (b) Calculate the wavelengths of the first three lines in the Balmer series - those for which \(n_{i}=3,4,\) and \(5-\) and identify these lines in the emission spectrum shown in Figure 6.11 .

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