Material Covered on Exam 3

Exam 3 will be held Wednesday, July 31 during the normal lecture period. The exam will consist of a combination of short-answer questions and problems similar to the assigned homework. A page of handwritten notes is allowed. No photocopies will be permitted. Any type of calculator is permitted, but using the programming feature to store equations is not. Makeup exams will be given only in the event of a previously approved excuse or an approved emergency.

You must have the symbol fonts installed to view Greek letters properly. You can download the file SYMBOL.TTF to your WINDOWS/FONTS folder if you do not have it already.


Background Material

You should remember the the basic relationships for linear motion (Chapter 2) and circular motion (Chapter 5), as well as the definitions of energy and momentum in Chapters 6 and 7. These concepts are a very basic part of physics and may appear throughout the course. If you need any thermodynamic relations, they will be given. All physical constants needed will be given.


Chapter 23, section 10

Concepts:

Combinations of lenses, geometric optics

Equations:

The thin lens equation relates the distances to the image and object, di and do to the focal length f according to

1/f = 1/di + 1/do .

The distance to the object and image are positive if they are real, and negative if they are virtual. The focal length is positive for converging lenses and negative for diverging lenses. The magnification of a lens is the ratio of the height hi of the image to the height ho of the object, and is given by

m = hi / ho = - di / do .
For combinations of lenses, the object position for the second lens is the image position for the first lens.


Chapter 25

Concepts:

Cameras, the eye, magnifiers, telescopes, microscopes, aberration, diffraction limits.

Equations:

Cameras:

f-stop = f/D

Eyes: Nearsightedness can be corrected by a diverging lens whose focal point is at the furthest point where the eye can naturally focus when relaxed. Farsightedness can be corrected with a converging lens which put the image of an object 25 cm away at the location of the eye's actual near point, which is further away. The thin lens equation is used in either case to find the focal length needed.

Magnifier: The magnification with the image at infinity is

M = N/f, with N = 25 cm
The magnification with the image at the near point N is
M = N/f + 1

In a telescope, parallel rays from a distant object are focused at the focal point of the objective lens, which is in turn the focal point of the eyepiece. Parallel rays then go to the eye, which sees the object at infinity.

Telescope with objective focal length fo and eyepiece focal length fi has magnification:

M = -fo/fi

In microscopes, the object is placed just beyond the focal point of the objective lens, producing an enlarged image at the focal point of the eyepiece, which acts as a magnifier to produce an image at infinity. The magnification of the objective lens is

mo = (L - fe)/do
The magnification of the eyepiece is
Me = N/f, with N = 25 cm.
The total magnification is
M = moMe.

The size of a lens aperture limits the resolution due to diffraction through the opening, which creates a peak whose half-width (width to first minimum) is

q = 1.22l / D.
The resolving power of a microscope is the smallest detail that can be seen, which has size
RP = f q = 1.22l/ D.

If a material of index of refraction n fills the space below the objective lens, the resolving power is smaller by a factor of 1/n, because the wavelength is increased by a factor of n compared to in a vacuum.

Units:

1 Diopter = 1 m-1 in inverse focal length


Chapter 26

Concepts:

The principle of relativity (physics is the same in all intertial frames), constancy of the speed of light in a vacuum, simultaneity, time dilation, length contraction, mass increase, relations between energy and momentum, addition of velocities.

Equations:

Let g = (1-v2/c2)-1/2. This factor is always greater than 1, and represents the time dilation factor by which events happen more slowly in a moving reference frame. A person taking a trip on a fast rocket will age more slowly by this factor. The mass of a moving object will increase by the same factor, and its length will decrease by this factor, becoming L / g.

The relativistic momentum is

p = mv = g mo v .

The kinetic energy of a moving object is

KE = (m-mo) c2
where mo is the rest mass and m is the relativistic mass. g mo.

The total relativistic energy satisfies

E2 = m2 c4 = p2 c2 + mo2 c4.

The relativistic sum of parallel velocities u and v is

(u + v) / (1 + uv / c2)
Units:

Convenient units for masses of relativistic particles are eV/c2. Convenient units of momentum are eV/c. For higher energies, substitute keV, MeV, ... as needed.


Chapter 27

Concepts:

Discovery of the electron, blackbody radiation and Planck's quantum hypothesis, the photoelectric effect and photons, photon interactions, wave-particle duality, the wave nature of matter (de Broglie waves), electron microscopes, early models of the atom, atomic spectra, the Bohr atom.

Equations:

There are many equations in this chapter. The following list contains some central ones, but is not complete. Please see the chapter for a complete list.

Planck's quantum hypothesis says that molecular or atomic vibrations have a minimum energy related to their frequency f by Emin = hf with Planck's Constant h = 6.626 x 10-34Js.

Photons are the basic particle constituents of electromagnetic fields. they carry energy

E = h f = h c / l
and momentum
p = E/c = h / l .

In the photoelectric effect, if is initially bound with a potential energy -W, which requires work W to overcome, then it is ejected from an atom with kinetic energy

KE = hf - W
where f is the frequency of the photon colliding with it.

de Broglie suggested that the relation between momentum and wavelength of photons applies to all objects: they have a wavelength related to their momentum by

l = h / p
This is confirmed by diffraction experiments with electrons.

Electron microscopes use the short wavelength of electrons to probe smaller objects than optical microscopes can.

The spectral lines of hydrogen have wavelengths given by the Rydberg law

1/l = R( 1/n12 - 1/n22 )
with n1 and n2 integers, and n2 > n1. R = 1.097 x 107 m-1 is the Rydberg constant. The series with n1 = 2 is the Balmer series, which begins in the visible range. The series with n1 = 1 is the Lyman series, and is in the UV range . The series with n1 = 3 is the Paschen series, and is in the IR range.

The spectral lines of single-electron atoms can be found using Bohar's quantum condition

mvr = nh / 2p
which leads to quantized orbital radii
rn = n2 rB/Z
where rB = 0.529 x 10-10 m is the Bohr radius and Z is the number of protons.

The quantized energy levels are given by

En = -13.6 eV x (Z/n)2

The spectral lines occur when the photon has an energy which is the difference between two of these quantized energy levels:

h f = En2 - En1
This is equivalent to the Rydberg law above for Hydrogen.


Physics 222 Department of Physics University of Tennessee