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Question: Incandescent lightbulbs heat up a filament 鈥渨hite hot,鈥 producing light of all wavelengths that has little to do with the filament鈥檚 composition. Gas vapor bulbs, such as sodium and mercury streetlights, produce colors that do depend on the gas in the bulb. Viewed with a diffraction grating (even a simple CD!), whereas the incandescent spectrum is continuous, that of a gas vapor (or fluorescent) bulb has characteristic lines. How is this indirect evidence of the wave nature of orbiting electrons?

Short Answer

Expert verified

Answer:

Only specific quantized energies are allowed for orbiting electrons, which leads to only specific wavelengths of photons. The electron should act like a wave inside the tiny constraints of the atom, creating quantized standing waves.

Step by step solution

01

The wavelength of a particle 

The wavelength of a particle can be obtained using the formula =hp=hmv.

02

Explanation

Gas vapor filaments, like sodium, form distinctive lines, or lines with particular wavelengths or energy. This indicates that, in accordance with the energy conservation principle, electrons either make the same transition across energy levels or exist in quantized states.

Bohr offered the theory that electrons behave as a wave that is contained in an orbit around the nucleus as one explanation. In accordance with this, some wavelengths (standing waves) can fit within these circles, much as how sound waves can fit inside of closed pipes or other musical instruments.

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Most popular questions from this chapter

The Moon orbits Earth at a radius of 3.84脳108m. To do so as a classical particle. Its wavelength should be small. But small relative to what? Being a rough measure of the region where it is confined, the orbit radius is certainly a relevant dimension against which to compare the wavelength. Compare the two. Does the Moon indeed orbit as a classical particle? (localid="1659095974931" mEarth=5.98脳1024kgand mmoon=7.35脳1022kg)

Question: Analyzing crystal diffraction is intimately tied to the various different geometries in which the atoms can be arranged in three dimensions and upon their differing effectiveness in reflecting waves. To grasp some of the considerations without too much trouble, consider the simple square arrangement of identical atoms shown in the figure. In diagram (a), waves are incident at angle with the crystal face and are detected at the same angle with the atomic plane. In diagram (b), the crystal has been rotated 450 counterclockwise, and waves are now incident upon planes comprising different sets of atoms. If in the orientation of diagram (b), constructive interference is noted only at an angle, =40at what angle(s) will constructive interference be found in the orientation of diagram (a)? (Note: The spacing between atoms is the same in each diagram.)

What is the range of frequencies in a 1 ns pulse of

(a) 1060nmInfrared laser light and

(b) 100MHzRadio waves?

(c) For which is the "uncertainty" in frequency, relative to its approximate value, larger?

All other things being equal, which would be more likely to exhibit its wave nature鈥攁 proton or an electron鈥攁nd why? By making something unequal, how could you 鈥渃ompensate,鈥 so as to make one as wavelike as the other?

In Exercise 45, the case is made that the position uncertainty for a typical macroscopic object is generally so much smaller than its actual physical dimensions that applying the uncertainty principle would be absurd. Here we gain same idea of how small an object would have鈾 to be before quantum mechanics might rear its head. The density of aluminum is 2.7103kg/m3, is typical of solids and liquids around us. Suppose we could narrow down the velocity of an aluminum sphere to within an uncertainty of1mper decade. How small would it have to be for its position uncertainty to be at least as large as110%of its radius?

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