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If particles have wavelike motion, why don't we observe that motion in the macroscopic world?

Short Answer

Expert verified
The wavelengths of macroscopic objects are too small to detect, making their wavelike motion unobservable.

Step by step solution

01

- Understand Wave-Particle Duality

Recognize that particles (like electrons) exhibit both particle and wave characteristics. This is known as wave-particle duality, a fundamental concept in quantum mechanics.
02

- Concept of De Broglie Wavelength

Identify that the wavelength associated with a particle is given by De Broglie's equation: \[\lambda = \frac{h}{p} \] where \(\lambda\) is the wavelength, \(h\) is Planck's constant, and \(p\) is the momentum of the particle.
03

- Calculate Wavelength for Macroscopic Objects

Notice that for macroscopic objects (e.g., a basketball), the mass and speed result in a very high momentum \(p\). Hence, the wavelength \(\lambda\) becomes extremely small and practically undetectable.
04

- Observation and Measurement

Acknowledge that the detection of wavelike motion requires the wavelength to be comparable to or larger than the size of the object or the scale of the measuring instrument. For macroscopic objects, the extremely small wavelength falls far below this threshold.
05

- Conclusion

Conclude that because the wavelengths of macroscopic objects are too small to be measured or observed with the naked eye or ordinary instruments, we perceive objects in the macroscopic world as having purely particle-like behavior.

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Key Concepts

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

Quantum Mechanics
Quantum mechanics is the branch of physics dealing with the behavior of very small particles, like electrons and photons. It differs significantly from classical physics, which describes the macroscopic world. In quantum mechanics, particles can display both wave-like and particle-like properties—a concept known as wave-particle duality. This duality enables particles to exist in multiple states at once, leading to phenomena like superposition and entanglement. These concepts, though mind-bending, are crucial for understanding the behavior of particles at the quantum level.
De Broglie Wavelength
The De Broglie wavelength is the wavelength associated with any moving particle and is given by the famous equation: \[ \lambda = \frac{h}{p} \] where \( \lambda\) is the wavelength, \( h\) is Planck's constant, and \( p\) is the momentum of the particle. This equation bridges the gap between the wave and particle nature of matter. Even particles with mass, like electrons, can exhibit wavelike behavior. The De Broglie hypothesis was revolutionary, showing that not just light but also matter has a dual wave-particle nature.
Macroscopic Objects
Macroscopic objects, like basketballs or even grains of sand, differ vastly from microscopic particles. In these larger objects, mass and velocity combine to result in enormous momentum. Applying the De Broglie equation, we find that the wavelength \( \lambda\) becomes incredibly tiny—far too small to be observed. This is why we don't notice wave properties in our everyday lives. The wave aspects of large objects are dwarfed by their particle characteristics, making them essentially invisible.
Planck's Constant
Planck's constant (symbolized as \( h\)) is a crucial term in the realm of quantum mechanics. Discovered by Max Planck, it’s valued approximately at \(6.626 \times 10^{-34} \ J \cdot s\), and it quantifies the scale at which quantum effects become significant. This constant appears in several core quantum mechanics applications, including the De Broglie wavelength formula. Its extraordinarily small value is the reason why the quantum effects are often not noticeable in our everyday macroscopic world.
Momentum
Momentum in physics is defined as the product of an object's mass and velocity, represented as \(p = mv\). For particles, high momentum means smaller wavelengths, according to the De Broglie formula. This relationship helps to explain why we don’t observe the wave-like behavior of larger objects. In the quantum world, where masses and velocities are typically extremely small, quantum effects and wave-like behaviors become observable. Thus, momentum plays a key role in differentiating the quantum realm from everyday experience.

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Most popular questions from this chapter

The photoelectric effect is illustrated in a plot of the kinetic energies of electrons ejected from the surface of potassium metal or silver metal at different frequencies of incident light. (a) Why don't the lines begin at the origin? (b) Why don't the lines begin at the same point? (c) From which metal will light of shorter wavelength eject an electron? (d) Why are the slopes equal?

The quantum-mechanical treatment of the hydrogen atom gives this expression for the wave function, \(\psi,\) of the \(1 s\) orbital: $$ \Psi=\frac{1}{\sqrt{\pi}}\left(\frac{1}{a_{0}}\right)^{3 / 2} e^{-r l a_{0}} $$ where \(r\) is the distance from the nucleus and \(a_{0}\) is \(52.92 \mathrm{pm}\). The probability of finding the electron in a tiny volume at distance \(r\) from the nucleus is proportional to \(\psi^{2}\). The total probability of finding the electron at all points at distance \(r\) from the nucleus is proportional to \(4 \pi r^{2} \psi^{2}\). Calculate the values (to three significant figures) of \(\psi, \psi^{2},\) and \(4 \pi r^{2} \psi^{2}\) to fill in the following table and sketch a plot of each set of values versus \(r .\) Compare the latter two plots with those in Figure \(7.17 \mathrm{~A}\).

Police often monitor traffic with "K-band" radar guns, which operate in the microwave region at \(22.235 \mathrm{GHz}\) ( \(1 \mathrm{GHz}=10^{9} \mathrm{~Hz}\) ). Find the wavelength (in \(\mathrm{nm}\) and \(\dot{\mathrm{A}}\) ) of this radiation.

How fast must a \(56.5-g\) tennis ball travel to have a de Broglie wavelength equal to that of a photon of green light ( \(5400 \mathrm{~A}\) )?

Which of these electron transitions correspond to absorption of energy and which to emission? (a) \(n=2\) to \(n=4\) (b) \(n=3\) to \(n=1\) (c) \(n=5\) to \(n=2\) (d) \(n=3\) to \(n=4\)

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