best pathway session: energy in k–12 physics...march 30, 2012 . energy savings •who will save...
TRANSCRIPT
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BEST Pathway Session: Energy in K–12 Physics
Arthur Eisenkraft
March 30, 2012
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Energy Savings
• Who will save more gasoline?
– Adam who switches from a gas-guzzler of 12 mpg to a slightly less voracious guzzler that runs at 14 mpg.
– The environmentally virtuous Beth switches from a 30 mpg car to one that runs at 40 mpg.
– Both travel equal distances over the year.
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The MPG Illusion
• Intuition – Beth’s action is more significant
• She reduced by 10 mpg rather than by 2 mpg
– Calculation • Adam: 10,000 miles will go from 833 gal to 714 gal
– A savings of 119 gallons
• Beth: 10,000 miles will go from 333 gal to 250 gal – A savings of 83 gallons
• Larrick and Soll showed that mpg is not as good as gallons/(100 miles) for these decisions – Study done in 2008 – Policy change expected in 2013 (in small print)
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Energy in Physics
• Energy in the new Framework for K-12 – Energy as a “disciplinary core idea”
– Energy as a crosscutting concept
• How do we present energy?
• Can we bring our presentations more in line with the 3-dimensions of the Framework – Scientific and Engineering Practices
– Crosscutting Concepts
– Disciplinary Core Ideas
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Types of Energy
• Please assist
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Types of Energy
• GPE • KE • SPE • Electrostatic PE • Heat • Light • Nuclear • Sound • Binding energy • Activation energy • Solar energy • Magnetic • Electrical
Equations for energy
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Types of Energy
• GPE mgh or –GMm/R • KE 1/2mv^2 • SPE ½ kx^2 • Electrostatic PE -kqq/R • Heat mc<delta>T • Light hf • Nuclear mc^2 • Sound • Binding energy • Activation energy • Solar energy • Magnetic • Electrical VIt
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Types of Energy Equation what we measure
• GPE mgh or –GMm/R • KE 1/2mv^2 • SPE ½ kx^2 • Electrostatic PE -kqq/R • Heat mc<delta>T • Light hf • Nuclear mc^2 • Sound • Binding energy • Activation energy • Solar energy • Magnetic • Electrical VIt
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Issues mentioned in the Framework
• The idea that there are different forms of energy, such as thermal energy, mechanical energy, and chemical energy, is misleading, as it implies that the nature of the energy in each of these manifestations is distinct when in fact they all are ultimately some mixture of kinetic energy, stored energy, and radiation.
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Issues mentioned in the Framework
• Furthermore, what is meant by the first three terms above is seldom precisely defined. It is likewise misleading to call sound or light a form of energy; they are phenomena that, among their other properties, transfer energy from place to place and between objects.
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Feynman’s 28 Blocks
• Day 1- 28 blocks; Day 2 – 28 blocks; etc.
• 27 (but one is under the couch)
• 25 (but box is heavier) – We can write an equation:
• (# of blocks seen) + (wt of box – 150 g)/20g = 28
• 26 (but water level in pail is higher) – We can write a new equation
• (# seen) + (weight…) + (ht of water – 2cm)/0.5 cm) = 28
• How else could blocks be hidden?
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Feynman’s 28 blocks
• 28 blocks
• One day – 30 blocks!!!!
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Energy Analogy
• First – a new level of abstraction – there are NO blocks
– Take away the first term in the equations
(# seen) + (weight…) + (ht of water – 2cm)/0.5 cm) = 28
• Second – Calculate energy (we don’t measure energy)
• Third – use the same units (Joules, calories, BTU, gallons of gas, eV….)
• Fourth – in a closed system – the sum is constant
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Conservation of Energy
• A closed system
• Different forms – each form has an equation – GPE, KE, elastic energy, heat energy, chemical
energy, radiant energy, nuclear energy
• The total of all of these numbers is constant.
• WE HAVE NO KNOWLEDGE OF WHAT ENERGY IS. We only know how to calculate energy and the total always remains the same.
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Our Faith in Energy Conservation
• Beta decay problems
– Energy was not conserved
• Wolfgang Pauli solution in 1931
– There must be a neutral particle unseen (neutron?)
– Chadwick discovers neutron in 1932 but is too massive for solution
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Our Faith in Energy Conservation
• Enrico Fermi in 1934 –theory of weak interactions – Neutrino with no charge, no mass
– But energy will be conserved
– Rejected by Nature ("it contained speculations too remote from reality to be of interest to the reader”)
• 1956 – the neutrino is experimentally discovered – Clyde Cowan and Fred Reines (Nobel Prize 1995) (Pauli
loses case of champagne in bet that it would never be detected)
• 1962 – not all neutrinos are identical
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How do we present energy?
• The Pole Vault
– The world’s record is 6.14 m (19.8 feet)
– Why not use a 7 meter pole and beat the record?
– How would you teach this?
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Energy in the Pole Vault
• Explore
– Investigate shooting
the penny in the air.
– Investigate bending
the flexible ruler.
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Energy in the Pole Vault
• Explain
– Speed of moving ball determines ruler bend
– Ruler bend determines height of penny
• Elaborate
ΔKE ΔEPE ΔGPE
• Pole length does not determine height
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Analysis of a Jump
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Analysis of a Jump
Elastic
Potential
Energy
Gravitational
Potential
Energy
Kinetic
Energy
ready position maximum 0 0
launch position 0 some maximum
peak position 0 maximum 0Po
siti
on
Energy
Qualitative treatment
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Analysis of a Jump
Elastic
Potential
Energy
Gravitational
Potential
Energy
Kinetic
Energy
ready position 410 J 0 0
launch position 0 150 J 260 J
peak position 0 410 J 0
Energy
Po
siti
on
Quantitative treatment
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Analysis of a Jump
Elastic
Potential
Energy
Gravitational
Potential
Energy
Kinetic
Energy
ready position 600 J 0 0
launch position 0 150 J 450 J
peak position 0 600 J 0Po
siti
on
Energy
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Analysis of a Jump on the Moon
Elastic
Potential
Energy
Gravitational
Potential
Energy
Kinetic
Energy
ready position 600 J 0 0
launch position 0 150 J 450 J
peak position 0 600 J 0Po
siti
on
Energy
Which values change?
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Analysis of a Jump on the Moon
Which values change?
Energy
Elastic Potential Energy Gravitational Potential
Energy Kinetic Energy
Po
siti
on
ready position 600 J 0 0
launch position 0 25 J 575 J
peak position 0 600 J 0
Since g is 1/6th on the moon, the corresponding height will be 6 x
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0.8 m 0.2 m
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5.0 m 0.8 m 0.2 m
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Sports on the Moon
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Popping Toy
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Popping Toy
0
100
200
300
400
500
600
700
beforepopping
just afterleaving the
table
halfway up at the top
Ene
rgy
(J)
Energy at different locations
Elastic Potential Energy (J)
Gravitational PotentialEnergy (J)
Kinetic Energy (J)
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Popping Toy
0
100
200
300
400
500
600
700
beforepopping
just afterleaving
the table
halfwayup
at the top
Ene
rgy
(J)
Energy at different locations
Elastic Potential Energy (J)
Gravitational PotentialEnergy (J)
Kinetic Energy (J)
0
100
200
300
400
500
600
700
beforepopping
just afterleaving the
table
halfway up at the top
Ene
rgy
(J)
Energy at different locations
Kinetic Energy (J)
Gravitational PotentialEnergy (J)
Elastic Potential Energy (J)
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Thermal Energy
• What is the final temperature when
– 100 g of water at 10° C is mixed with
– 100 g of water at 50°C ?
• Student “incorrect” response is often 40° C
– How do they get this?
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Thermal Energy
• What is the final temperature when
– 100 g of water at 10° C is mixed with
– 100 g of iron at 50°C ?
0 10 20 30 40 50 60 70 80
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Thermal Energy
• What is the final temperature when
– 100 g of water at 10° C is mixed with
– 100 g of iron at 50°C ?
• Experimental answer = 22°C
• How can our students explain?
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Thermal Energy
• What is the final temperature when
– 100 g of water at 10° C is mixed with
– 100 g of water at 50°C ?
• Conservation of Energy
– Energy gain of the cold water = Energy loss of the hot water
– Energy change of the cold water + energy change of the hot water = 0
– Total energy remains constant
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Thermal Energy
• What is the final temperature when
– 100 g of water at 10° C is mixed with
– 100 g of iron at 50°C ?
• Experimental answer = 22°C
• Conservation of Energy
– Energy gain of the cold water = Energy loss of the iron OR Total energy remains constant
• Water requires more energy to change its temperature definition of specific heat
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Energy as a Crosscutting Concept
Traditional Lesson with Disciplinary Core Ideas in Foreground
Revised Lesson with Crosscutting Concepts in Foreground
Place hot iron in cold water and heat up water Place hot iron in cold water and heat up water
Research Question: Find the specific heat of the iron.
Research Question: Is energy conserved?
Measure the temperature gain of the water. Calculate the energy gain of the water.
Measure the temperature gain of the water. Calculate the energy gain of the water.
Assume that energy is conserved Calculate the energy loss of the iron using the Handbook value.
Determine the specific heat of the iron. Determine if energy is conserved
Compare the calculated specific heat of the iron with the “correct” value in the Handbook .
Account for the loss of energy (the energy loss of the iron is greater than the energy gain of the water.)
Calculate the percent error. Account for this percent error.
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Energy as a Crosscutting Concept
• We pulled off the internet the first 23 sets of lab instructions for this lesson. In only 7 of these lesson descriptions and handouts did we find any mention of either “energy conservation (1 lab),” “conservation of energy (3 labs),” “law of conservation of energy (1 lab),” or “energy loss = energy gain (2 labs).”
• No other explicit phrases for conservation of energy (e.g. total energy remains constant) were found. In the remaining 16 sets of instruction, the conservation of energy is implied and used but never stated.
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Relevance of Thermal Energy
• What way to heat water uses least energy?
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Relevance of Thermal Energy
• What is the best way to cook a hot dog? – Fry, boil, microwave, grill
• Define “best” – Fastest
– Cheapest
– Least cleanup
– Best taste
– Best appearance
• Engineering Design
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Energy in Physics
• Energy in the new Framework for K-12 – Energy as a “disciplinary core idea”
– Energy as a crosscutting concept
• How do we present energy?
• Can we bring our presentations more in line with the 3-dimensions of the Framework – Scientific and Engineering Practices
– Crosscutting Concepts
– Disciplinary Core Ideas
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Energy in Physics
• Energy in the new Framework for K-12 – Energy as a “disciplinary core idea” – Energy as only one crosscutting concept
1. Patterns
2. Cause and effect: Mechanism and explanation
3. Scale, proportion, and quantity
4. Systems and system models
5. Energy and matter: Flows, cycles, and conservation
6. Structure and function
7. Stability and change
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Conservation of Energy
• A closed system
• Different forms – each form has an equation – GPE, KE, elastic energy, heat energy, chemical
energy, radiant energy, nuclear energy
• The total of all of these numbers is constant.
• WE HAVE NO KNOWLEDGE OF WHAT ENERGY IS. We only know how to calculate energy and the total always remains the same.
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• Please check out our website: www.umb.edu/cosmic
for a copy of the power point.
Or email with questions: [email protected]
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A Falling Object
• How do we determine it’s path – Kinematics equations
• vf = at + vi • • vf
2= 2ad + vi2
• • vf = aΔt + vi • • y= ½ at2 + vit • • Δy = vΔt
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Least Action
• Calculate the Lagrangian, L = T - V, at several instants (t), and draw a graph of L against t. The area under the curve is the action. Any different path between the initial and final positions leads to a larger action than that chosen by nature. Nature chooses the smallest action - this is the Principle of Least Action.
• Total energy = T + V • • 6.2 The principle of stationary action • Consider the quantity, • S ´ • Z t2 • t1 • L(x; x_ ; t) dt: (6.14) • S is called the action. It is a quantity with the dimensions of (Energy)£(Time). S depends • on L, and L in turn depends on the function x(t) via eq. (6.1).4 Given any function x(t), • we can produce the quantity S. We'll just deal with one coordinate, x, for now. • • • • •