PreLecture : Rutherford Simulation

54
PreLecture: Rutherford Simulation Turn on the “Show Traces option, and simply show the Phet: http ://phet.colorado.edu/en/simulat ion/rutherford- scattering

description

PreLecture : Rutherford Simulation. Turn on the “ Show Traces ” option, and simply show the Phet : http ://phet.colorado.edu/en/simulation/rutherford- scattering. Mr. Klapholz Shaker Heights High School. Atomic and Nuclear Physics (7). - PowerPoint PPT Presentation

Transcript of PreLecture : Rutherford Simulation

Page 1: PreLecture : Rutherford Simulation

PreLecture: Rutherford SimulationTurn on the “Show Traces” option, and simply show the Phet:http://phet.colorado.edu/en/simulation/rutherford-scattering

Page 2: PreLecture : Rutherford Simulation

Atomic and Nuclear Physics (7)

Humans have been thinking about atoms for thousands of years. The biggest surprise about

atoms is that they do not behave at all like regular-sized objects. The objects in your world

operate according to familiar patterns of Newton, but the particles that make up your

world do not operate by those rules.

Mr. KlapholzShaker Heights

High School

Page 3: PreLecture : Rutherford Simulation

Atoms, Pre-Rutherford In the year 1900, people had evidence that atoms existed, and that there was positive and negative charge, but there was almost no idea about how atoms were built of charge.

Page 4: PreLecture : Rutherford Simulation

Raisin Bun

http://kristinasjollyhockeysticks.blogspot.com/2009_03_01_archive.html

Page 5: PreLecture : Rutherford Simulation

Plum Pudding or

Raisin Bun Model of the atom

One idea was that the electrons were in a positive goop, like plums in pudding, or like raisins in a pastry.

http://mnhs.wikispaces.com/School+Forum

Page 6: PreLecture : Rutherford Simulation

Rutherford• Then came one of the biggest experiments in

human experience. • In short, it told us that: the atom’s mass was

concentrated in an ultra-dense speck of a positive nucleus, the negative electrons formed the outer part of the atom, and in between the electrons and the nucleus was… nothing.

• This was nothing like plum pudding or raisin bread.

http://elements.vanderkrogt.net/element.php?sym=Rf

Page 7: PreLecture : Rutherford Simulation

How did Rutherford figure out so much?

Page 8: PreLecture : Rutherford Simulation

Rutherford, Geiger, Marsden

http://reich-chemistry.wikispaces.com/stephen.gasecki.timothy.graham.atomichistory.fall.2009

of alpha particles

Page 9: PreLecture : Rutherford Simulation

The alpha(positive, massive, fast)

Page 10: PreLecture : Rutherford Simulation

Data

• Almost every alpha particle goes through the gold foil unaffected by the gold.

• Those very few alpha particles that are affected by the foil are deflected a lot.

Page 11: PreLecture : Rutherford Simulation

Gold atom and alpha particles

http://www.clemson.edu/caah/history/facultypages/PamMack/lec122sts/invention14.html

Page 12: PreLecture : Rutherford Simulation

Conclusions of Rutherford’s experiment

• Most of the alpha particles are not affected by the gold foil. This tells us that most of an atom is empty.

• The few particles that bounced back must have been forced by a positive massive object. That’s what we now call the nucleus.

• And that’s how things stayed for 4 years: atoms had a massive positive part, and a negative part, but we didn’t know how it all fit together.

Page 13: PreLecture : Rutherford Simulation

Niels Bohr was able to come up with a model that made sense of just about everything:

• The electrons were light, negative particles that orbit the nucleus.

• The reason that atoms are mostly empty is that electrons zing around in paths that are much bigger than a nucleus.

• Like the planets orbiting the sun, the electrons were attracted to the nucleus.

• For any circular orbit, the force is toward the center. For electrons, it’s the attractive force between positive and negative that provides that force.

Page 14: PreLecture : Rutherford Simulation

Electron Orbits

http://wisp.physics.wisc.edu/astro104/lecture6/lec6_print.html

Page 15: PreLecture : Rutherford Simulation

More on Bohr

• Bohr predicted energy orbits (“orbitals”). An electron could only exist in particular orbits.

• When an electron went from high energy (say n = 4) to lower energy (say n=1), the electron would emit light.

• The greater the energy drop, the greater the frequency of the light: hf = DE.

• h = 6.6 x 10-34 m2 kg s-1 = 6.6 x 10-34 J s

Page 16: PreLecture : Rutherford Simulation

How to measure emission spectrum

http://www.tutornext.com/help/emission-spectra

Page 17: PreLecture : Rutherford Simulation

Absorption spectrum apparatus.The white light starts on the right, goes through

the gas, and is observed on the left.

http://physics.kenyon.edu/EarlyApparatus/Optics/Sodium_Absorption_Spectrum/Sodium_Absorption_Spectrum.html

Page 18: PreLecture : Rutherford Simulation

Emission spectrum is on the top. Absorption spectrum is on the bottom.

http://www.cbu.edu/~jvarrian/252/emspex.html

Why are only specific colors emitted / absorbed by hydrogen?

How do the emitted colors relate to the absorbed colors?

Hydrogen

Hydrogen

Hydrogen

Hydrogen

Page 19: PreLecture : Rutherford Simulation

Photon Basics• A photon is a particle of light.• A photon is a bundle of energy with a specific

frequency. High frequency goes with high energy: E = hf.

• Light acts as a wave. Light acts as a particle. Particles are very different from waves. “Duality.”

• Bright light has more photons than dim light.

Page 20: PreLecture : Rutherford Simulation

Photons and Atoms• When an electron drops from a high energy level

to a low level, the atom emits a photon; the energy of the photon equals the energy difference of the electron levels.

• When an atom absorbs light, an electron goes from a low energy level to a high level. The energy of the absorbed photon equals the energy difference of the electron levels. The only photons that an atom can absorb are the ones that match the differences in electron energy levels.

Page 21: PreLecture : Rutherford Simulation

Ions

• If an atom loses an electron, then the atom is charged. Will it be positive or negative?

• A charged atom is called an ion.• The energy required to remove an electron is

called the ionization energy.

Page 22: PreLecture : Rutherford Simulation

The Electron VoltHow much energy would an electron gain if we

let a 1-Volt battery give it a boost? • Voltage = Energy / Charge• Energy = Voltage x Charge• Energy = (1 V) x (1.602 x 10-19 C)• E = 1.602 x 10 x 10-19 J • 1 electron-Volt = 1.602 x 10-19 J …1 eV = 1.602 x 10-19 J (It is a unit of energy)

Page 23: PreLecture : Rutherford Simulation

Planck’s constant

• As you know, h = 6.626 x 10-34 J s • Also, h = 4.136 x 10-15 eV s

Page 24: PreLecture : Rutherford Simulation

Easy Problem Solving• If an electron is in the 2nd orbital (19 eV) and

drops to the first orbital (10 eV), then what is the frequency of the photon that is emitted?

Solution:DE = 9 eVDE = hf

f = DE ÷ h f = (9 eV) ÷ (4.136 x 10-15 eV s )

f = 2 x 1015 Hz

Page 25: PreLecture : Rutherford Simulation

Spot the nucleus

http://student.ccbcmd.edu/~cminnier/radioact1/121radio3.htm

Page 26: PreLecture : Rutherford Simulation

The Nucleus (1 of 2)• There are protons in the nucleus– Charge = +1.602 x 10-19 C– Mass = 1.673 x 10-27 kg

• There are neutrons in the nucleus– Charge = 0– Mass = 1.675 x 10-27 kg

• Notice that the charge of the proton is equal (in size) to the charge of the electron.

• Notice that neutrons are just a wee bit more massive than protons. (It is almost as if neutrons had a proton and an electron inside.)

Page 27: PreLecture : Rutherford Simulation

The Nucleus (2 of 2)• Nucleon – the name for protons and neutrons.

Protons are nucleons, and neutrons are nucleons. The number of nucleons is symbolizes by A.

• Atomic Number (Z) – This is the number of protons in the nucleus. This is the only thing that makes an atom be a particular element. For example, all atoms of oxygen have 8 protons.

• Isotopes – Two atoms of the same element can have different numbers of neutrons (N) and therefore different masses.

Page 28: PreLecture : Rutherford Simulation

A problem

• Hey, what holds the nucleus together in such a small space?

• What holds a neutron to another neutron?• And, … WHAT COULD POSSIBLY HOLD A

PROTON SO CLOSE TO ANOTHER PROTON?

Page 29: PreLecture : Rutherford Simulation

The Strong Force

• The third force that we know of is the force that holds nucleons together in the nucleus.

• This force is extremely short range, and unbelievably intense.

• Because of the strong force, it is pretty tough to get the nucleons in a nucleus to come apart.

• Once a nucleon is out of the nucleus, this force has no effect on it.

Page 30: PreLecture : Rutherford Simulation

Mass of a Nucleus

• If you add up the masses of the nucleons before they are together, you get a slightly greater value than if you measure the mass of the whole nucleus.

• The difference is called the mass defect.

Page 31: PreLecture : Rutherford Simulation

Binding Energy

• If you multiply the mass defect by the speed of light squared, you get the energy required to break apart the nucleus.

• E = mc2.• The bigger the nucleus, the greater the

binding energy. (It takes more energy to separate all those nucleons.)

• But what if you graphed B.E. per nucleon vs size of nucleus?

Page 32: PreLecture : Rutherford Simulation

The binding energy curve

http://library.thinkquest.org/3471/mass_binding.html

Page 33: PreLecture : Rutherford Simulation

Why do nuclei move toward iron (56)…?

http://www.google.com/imgres?imgurl=http://www4.nau.edu/meteorite/Meteorite/Images/BindingEnergy.jpg&imgrefurl=http://www4.nau.edu/meteorite/Meteorite/Book-GlossaryB.html&h=459&w=567&sz=37&tbnid=2l4x3t2tTYh6pM:&tbnh=108&tbnw=134&prev=/images%3Fq%3Dbinding%2Benergy%2Bcurve&zoom=1&q=binding+energy+curve&hl=en&usg=__yHj4cmQEXQXAHu4tw_7fByoPI3s=&sa=X&ei=CXHdTM--Kse1nweDorCDDw&ved=0CCQQ9QEwBA

Page 34: PreLecture : Rutherford Simulation

Big nuclei get smaller, and small nuclei combine.

http://www.google.com/imgres?imgurl=http://www4.nau.edu/meteorite/Meteorite/Images/BindingEnergy.jpg&imgrefurl=http://www4.nau.edu/meteorite/Meteorite/Book-GlossaryB.html&h=459&w=567&sz=37&tbnid=2l4x3t2tTYh6pM:&tbnh=108&tbnw=134&prev=/images%3Fq%3Dbinding%2Benergy%2Bcurve&zoom=1&q=binding+energy+curve&hl=en&usg=__yHj4cmQEXQXAHu4tw_7fByoPI3s=&sa=X&ei=CXHdTM--Kse1nweDorCDDw&ved=0CCQQ9QEwBA

Page 35: PreLecture : Rutherford Simulation

Radioactive Decay (big nuclei get smaller)

• Big nuclei are not stable. They come apart naturally.

• There are three kinds of radiation, named for the first three letters of the Greek alphabet:– Alpha– Beta– Gamma

Page 36: PreLecture : Rutherford Simulation

Meet the Alpha (42a = 4

2He) again

Page 37: PreLecture : Rutherford Simulation

Alpha particles…

• are the nuclei of helium atoms.• have a lot of energy, so even one alpha can

ionize many atoms.• are a health hazard, due to their ability to ionize

atoms in living tissue.• are easy to detect, due to their ability to ionize.• are easy to stop, due to the amount of energy

that they lose when ionizing atoms.

Page 38: PreLecture : Rutherford Simulation

Alpha decay

• Makes the nucleus drop in mass by about 4 mass units.

• Makes the nucleus drop in atomic number (Z) by 2 charge units. The atom literally changes from one element to another.

Page 39: PreLecture : Rutherford Simulation

Beta particles (b- = 0-1b = 0

-1e = e-)

• are pretty much the same as electrons• have low mass, so they are not very effective

at ionizing atoms• have a lot of energy so they are easy to

measure.• are difficult to stop.

Page 40: PreLecture : Rutherford Simulation

Beta Decay

http://www.green-planet-solar-energy.com/nuclear-power-information.html

Page 41: PreLecture : Rutherford Simulation

Beta Decay

http://education.jlab.org/glossary/betadecay.html

The nucleus gets a wee bit less massive, and it becomes more positively charged. (An antineutrino is also released.)

Page 42: PreLecture : Rutherford Simulation

Neutrinos and Antineutrinos

• Ultra low mass.• Almost never react with matter.• Hard to detect.

Page 43: PreLecture : Rutherford Simulation

Gamma (g = 00g) radiation

• This is pure electromagnetic energy. (Light is an example, and so are x-rays.) E = hf.

• When a gamma ray leaves any object (including a nucleus) the object is left with less energy.

• The mass does not change.• The charge does not change.

Page 44: PreLecture : Rutherford Simulation

Comparison tableAlpha Beta Gamma

Range in air About 5 cm About 30 cm About 100 cmPenetration Stopped by

paperStopped by thin layer of lead, or even aluminum foil

Stopped by thick layer of lead

Ionization ability

High Low Moderate

Detection GM tubeCloud chamberPhotographic paper

GM tubeCloud chamberPhotographic paper

GM tubeCloud chamberPhotographic paper

Page 45: PreLecture : Rutherford Simulation

Nuclear Radiation and Health

• Good: X-rays, treatment of cancer• Bad: causes mutations and cancer (In

high doses radiation kills quickly).• Protection: distance (1/R2) and shielding

http://www.sciencedaily.com/articles/mind_brain/steroids/5/

Page 46: PreLecture : Rutherford Simulation

Half Life (T½)• Which leaf will fall next?• Do the leaves fall more

often when there are more on the tree, or less on the tree?

• How often do the leaves fall?

• How much time will it take until all the leaves have fallen off?

http://www.istockphoto.com/stock-illustration-10466423-autumn-tree-with-falling-leaves.php

Page 47: PreLecture : Rutherford Simulation

Half Life (T½)

• In a sample of uranium, which nucleus will decay next?

• Do the nuclei decay more often when there are more uranium nuclei, or when there are less?

• How often do the nuclei decay?• How much time will it take until all the nuclei

have decayed?

Page 48: PreLecture : Rutherford Simulation

Half Life (T½)

• Although we do not know when all of the nuclei will have decayed, the time for half to decay is a reasonable quantity to measure. It works for trees, nuclear fission, and even the level of caffeine in a teacher’s blood.

• Any single urananium nucleus has a specific probability of decaying in the next second.

Page 49: PreLecture : Rutherford Simulation

The rate of decay is proportional to the number of nuclei that

have not yet decayed.

Page 50: PreLecture : Rutherford Simulation

Decay Curve1) When have all of the nuclei decayed?

http://www.tutorvista.com/physics/radioactive-decay-physics

Page 51: PreLecture : Rutherford Simulation

2) Half life is defined as the amount of time for half of the nuclei to decay.

http://www.tutorvista.com/physics/radioactive-decay-physics

Page 52: PreLecture : Rutherford Simulation

The rate at which the nuclei decay is the gradient of the decay curve. Try sketching it. It is

called “Activity”. What are the units?

http://www.tutorvista.com/physics/radioactive-decay-physics

Page 53: PreLecture : Rutherford Simulation

Nuclear Reactions - Fission(big nuclei get smaller)

• Big nuclei (such as uranium and plutonium) are not as stable as medium-sized nuclei, so they come apart.

• During fission, the Binding Energy per nucleon will increase, leaving a more stable nucleus.

• This type of reaction happens in the nuclear power plant in Perry, OH, 38 miles from here.

http://watergatesummer.blogspot.com/2007_11_01_archive.html

Page 54: PreLecture : Rutherford Simulation

Nuclear Reactions - Fusion(small nuclei get bigger)

• Small nuclei are not as stable as medium-sized nuclei, so these nuclei join together when given the chance.

• During fusion, the Binding Energy per nucleon will increase, leaving a more stable nucleus.

• This type of reaction happens in the sun. Fusion research is intense, with the hope of making cleaner nuclear energy here on earth.