9.4 Towards absolute zero

At absolute zero,

A Reversible process is

a process which can be made to go in the reverse direction by an infinitesimal change in the conditions which are causing it took take place.

Latent heat (L)

is defined as the amount of energy required to break bonds. L is the DQ you need to put into a system in order to melt/vaporise it. It goes into both DU and DW. The material will expand or contract due to the change, so DW 0. DU 0 either, because the internal potential energy will increase as well (not the internal kinetic energy though).

Specific latent heat of fusion (l)

The heat of fusion per unit mass. Units: J kg-1.

Ideal gas laws apply least at

(when the gas is close to liquefaction)

Real gases have intermolecular forces and their molecules have volume.

Andrews' experiment

compared CO2 and N2 gases. N2 nearly ideal at the T, p he was using.

--> Volume

Important things about the apparatus:

Critical temperature Tc  

Above the critical temperature Tc (31.1OC for CO2) a substance is always a gas. It is not possible to liquefy it by compression. Below this point a substance can exist as an unsaturated vapour (technical term for a substance in gas phase below Tc), a liquid, or an equilibrium mixture of the two.

Critical pressure pc

The minimum pressure at which a gas can be liquefied at Tc. (This is the top of the darker grey curve).

Specific critical volume

The volume of a gas at it's Tc and pc .

The liquid and it's saturated vapour have the same volume at this point, and so have the same density. There is no meniscus- and therefore no distinction between liquid and vapour.


Boyle temperature

The temperature at which the gas's behaviour is closest to an ideal gas, ie. Increasing p has little (ideally no) effect on pV.

This is TB on the left hand graph of pV against p.

Evaporation

is the process by which a liquid becomes a gas.

Rate of evaporation depends on surface area, temperature, air movement around the surface (the more the better) and air pressure (the lower the better). Evaporation cools a liquid because the molecules with the highest EK are lost first, so average EK drops.

Fridge

Freon has TC > room temperature, so it can be liquefied at room temperature by compression. 

Pump -> cooling fins -> valve -> inside of fridge -> pump.

Joule-Kelvin effect

A temperature change occurs when a gas at one constant pressure is forced through a hole into a region at a constant, lower pressure. The gas expands quickly on reaching the other side: no heat is put in or removed, so this is adiabatic expansion.

Superconductors

Gold, Silver, Copper, and ferric metals do not superconduct.

Other metals, and some ceramics, do superconduct:


Values of Bc and Jc are found for 0K (maximum).

Superfluids

Helium 4 is a superfluid below 2.17K (the lambda point, Tl) . Below this point it acts like a mixture of two liquids: a normal liquid, and a superfluid. It is called Helium II (instead of Helium I, it's when a liquid name above this point (2.17 to 4.2K)).

 

 

9.3 Special Relativity

Michelson-Morley experiment

Ways to explain the result

  1. The ether is dragged along by the Earth. The phenomenon of stellar aberration disproves this.

  2. Light always travels at the same speed with respect to it's source. This was rejected because this would make light unique - no other wave motions do this.

  3. Objects moving through the ether with velocity v contract in the direction of their motion by a factor (1 - v2/c2) - Fitzgerald-Lorentz contraction.

So either

Both of which leads to the conclusion that

Inertial Frame

An inertial frame is one where Newton's First Law is valid.

Law 1: if no resultant force acts on a body, it's velocity will not change.

(F=0, therefore Dv = 0)

Special relativity

Based on two postulates:

  1. Physical laws have the same form in all inertial frames of reference. (the principle of special relativity)

  2. The speed of light (in vacuum) is the same in all inertial frames. It does not depend on the velocity of the source or the observer.

So an experiment performed in one inertial frame will have the same result in any other inertial frame. No one frame is at rest. All motion is relative.

Time dilation

Length contraction

Relativistic mechanics

Relativistic momentum = mv = m0v / (1 - v2 / c2 )

Total energy of a body = rest energy + relativistic kinetic energy

The rest energy is simply m0c2.

The total energy is mc2.

From these, the relativistic kinetic energy can be found:

K = mc2 - m0c2

When v << c, K = m0v2.

Photon in a Box

For the photon in a box derivation, you need to know

Use conservation of momentum to work out how the photon mass relates to the photon energy. Comes out as E=mc2.

Confirmation

 

9.2 Wave particle duality

Huygens' wave theory was less popular because

even though beams of light could cross without interfering with each other.

 

Newton's particle theory of light said that

It was disproved by

 

Maxwell

Maxwell proposed that, since a changing magnetic field caused a changing electric field and vice versa, an EM wave consisting alternately of both could propagate through space. A B-field causes an E-field causes a B-field and so on. 

He predicted the wave speed as c = 1 / (m0e0). This gave a value close to the known value of c.

Hertz

Discovered radio waves. Used a spark gap transmitter and a wire loop receiver to do this. The transmitter is effectively a high frequency resonator. The plates are charged by the induction coil, and the charge is dissipated through the resistance between the air gaps when the spark occurs. At this point, a high frequency a.c. current flows in the circuit. This resonance frequency is the same as the frequency of the EM waves emitted.

Hertz could only detect the waves when his receiver was pointing at them (don't know which way round that is) and thus found they were polarised as Maxwell had suggested. He also set up a standing wave and found the wavelength (distance between two nodes is half a wavelength).

Michelson 1926 (finding c accurately)

Rotating octagonal prism on Mt. Wilson.

Black body

A black body absorbs all the radiation incident upon it. It is also a good radiator (good absorber = good emitter). The box with matt black insides comes close to this in practice. A black body emitter uses such a box. Since most of the radiation produced by the inside of the box is absorbed by other parts, the radiation output is a mixture of radiation from all over the inside of the box. There are no problems due to hot spots or cold spots.

Black body spectrum

Found using black body radiator, two concave mirrors, a slit and fluorspar prism. The concave mirrors produce parallel or nearly-parallel radiation. The prism splits the radiation up so that it can be measured using a linear bolometer: strip of Pt foil, painted black. Resistance changes with temperature, so a Wheatstone bridge is used to find the resistance and from it the magnitude of radiation with a particular wavelength. You can get a radiation spectrum for emissions from a black body at a particular temperature.


Wien's displacement law: lmax = constant

Stefan's law: Total energy radiated E = sT 4

s is Stefan's constant.

Classical physics could only explain black body radiation in terms of each part of the black body radiating energy of any wavelength. The Rayleigh-Jeans formula was based on classical physics and is correct for large l, but incorrectly tends to infinity for small l.

Planck found a correct formula from experimental results: Planck's radiation law. It was impossible to justify this in terms of classical physics. Planck concluded that the known laws of physics did not necessarily apply on an atomic scale. He proposed instead that energy can be absorbed or radiated only in discrete packets: quanta, each of energy hf. This was the beginning of the quantum theory, as it implies that the energy of a system can only change in discrete amounts.

h = Planck's constant

Boltzmann's constant, by the way, is the ratio R / L (L = Avogadro's number).

Einstein's photoelectric theory  1905

Lenard did some experiments around 1900 in which he researched the effect, which had been discovered by Hertz, and discovered a few things about it which could not be explained by the classical physics "wave theory" of light. This stated that light energy would be distributed equally to all the atoms on the surface, and therefore that electron emission should depend only on intensity. Einstein's theory was drawn up to explain why the photoelectric effect would not occur below a particular frequency of light, and why the e- emitted had a kinetic energy dependant on the light frequency.

hf = F + mv2

Millikan's experiment was a more careful test of the theory. Based on using an electric field to stop the photoelectrically emitted electrons. The p.d. was adjusted to find the point where it was just enough to stop the electrons. (work done by electron against a p.d. = energy lost by electron due to deceleration = eV). From this Millikan found the k.e. of the electrons and was able to plot a graph of light frequency against electron energy for a few metals (Li, K, Na). He also found the work function of these metals which turned out to be close to the one for thermionic emission, and found an accurate value of h.

De Broglie

Suggested that, as light could be considered as consisting of photons, each of energy hf, then matter might also have a wavelength.

For a photon:

E = hf and p = E/c

E = cp = hf therefore p = hf / c

But c / f = l. So p = h / l.

De Broglie's hypothesis was that a particle of momentum p will have wavelength l. This is now called the de Broglie wavelength.

From this, it follows that matter can be diffracted, and Davisson and Germer succeeded in diffracting electrons. Later experiments found that it was possible to diffract neutrons, protons, H and He atoms.

Davisson and Germer used a technique similar to that used for X-ray diffraction to look at electron diffraction patterns. They fired beams of electrons at Ni crystals- the beams were diffracted by the atoms. The pattern was analysed using a Faraday cylinder as a collector.

GP Thomson used very thin metal foils and a photographic plate to show electron diffraction. The polycrystalline (randomly structured) foil produced ring patterns- with the same wavelength predicted by de Broglie.

The wavelength of an electron is l = h /(2meV)

(proved using k.e. formulae for electrons, and p = mv = h / l )

Madness

The waves do not really exist: except in terms of probability. The amplitude of a wave at a particular point in space is found by the wave function Y, where Y is a function of x, y, z and t. eg. amplitude = Y(x,y,z,t). The square of this amplitude is the probability of the particle being at this point, at this time.

The probability of a photon of light being at a particular point depends on the light intensity at that point, which depends on the amplitude of the electric field vector.

So a particle cannot be said to be at one particular point: the probability will be non-zero for a small region of space in all cases.

Electron microscopes

The TEM has a greater resolving power than the best theoretical optical microscope, because the de Broglie wavelength of the electrons it uses is less than the minimum wavelength of blue light. (Optical can resolve objects 2 x 10-7 m apart, electron can theoretically resolve objects 2 x 10-12 apart).

But...

Process: gun -> condenser -> object -> objective -> projector -> final image

The STM uses electron tunnelling. As an electron can be treated as a wave, there is a possibility of it being at any point around the point where it is most likely to be. It can even cross potential energy barriers if there is a possibility of it being on the other side. This allows electrons to jump the gap between the surface being investigated and the STM probe. The current is maintained by moving the probe up and down as the surface is scanned, to trace a map of surface.

this version 0.0.1 - was taken and adapted from a web search - I forget where I found it - but acknowledgements go to whoever.

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