Physics I 95.141 LECTURE 13 10/20/10

36
rtment of Physics and Applied Physics 95.141, F2010, Lecture 13 Physics I 95.141 LECTURE 13 10/20/10

description

Physics I 95.141 LECTURE 13 10/20/10. Circular Motion Problem. (A) What is the centripetal acceleration/Force of/on the bullet? (5pts) (B) Where does this Force come from? (95 pts). Circular Motion Problem. R~1300m m bullet =.03kg v bullet =300m/s. 40m. 0.15m. Lecture 12 Review. - PowerPoint PPT Presentation

Transcript of Physics I 95.141 LECTURE 13 10/20/10

Page 1: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Physics I95.141

LECTURE 1310/20/10

Page 2: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Circular Motion Problem

• (A) What is the centripetal acceleration/Force of/on the bullet? (5pts)

• (B) Where does this Force come from? (95 pts)

Page 3: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Circular Motion Problem

• R~1300m• mbullet=.03kg

• vbullet=300m/s0.15m

40m

Page 4: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Lecture 12 Review• Translational Kinetic Energy

• Work Energy Theorem– The net work done on an object corresponds to the change in

translational kinetic energy of that object (as long as this energy does not go into internal energy…compressed spring, for instance)

• Conservative vs. Non-Conservative Forces– The work done by a conservative force to move an object from

point A to B depends only on the position of A and B, not path or velocity.

2

21mvKE

21

22 21

21 mvmvKEWWnet

Page 5: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Potential Energy

• In the last class we defined Energy as the ability to do work.

• In particular, we discussed Translational Kinetic Energy, the energy associated with motion.

• However, there are numerous other types of Energy– We know batteries can do work– We know a coiled spring can do work– We know a mass at some height, attached to a pulley can do

work

• All of these are examples of systems that have the potential to do work, and we can associate with them a potential energy.

Page 6: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Gravitational Potential Energy

• Say we start with a mass, and raise it, at constant velocity, to a height h.

• How much work do we do?

• How much work does gravity do?

Page 7: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Gravitational Potential Energy

• The block now has the potential to do work….• Say we drop the brick, at y=0, we can find the

Kinetic Energy of the brick by the work-energy theorem:

Page 8: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Gravitational Potential Energy

• At y=0, the block can do an amount of work equal to it’s kinetic energy

• Imagine the brick being used to drive a stake into the ground:

Page 9: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Gravitational Potential Energy

• Summary– Raising the brick gives it the potential to do work, that

potential energy is given by:

– As the brick falls, its potential energy is converted into kinetic energy

Page 10: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Gravitational Potential Energy

• We assign the letter U to the gravitational potential energy

• The change in gravitational potential energy is then:

Page 11: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Gravitational Potential Energy

• The gravitational potential energy is associated with the Force between the Earth and the object.

• How do we determine what y is?

• It is the change in Potential Energy that we are usually concerned with

Page 12: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Example Problem• A 1000kg roller coaster moves from point 1 to points 2 and 3. • What is the potential energy of the roller coaster at points 2 and 3

relative to point 1?• What is the change in potential energy from points 2 to 3?

Page 13: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Example Problem• A 1000kg roller coaster moves from point 1 to points 2 and 3. • What is the potential energy of the roller coaster at points 2 and 3

relative to point 3?• What is the change in potential energy from points 2 to 3?

Page 14: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

General Potential Energy

• Gravitational potential energy is defined as:– The negative of the work done by gravity when the

object moves from height y1 to y2.

• In general, we can define the change in potential energy associated with a particular Force F as the negative of the work done by that Force.

Page 15: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Elastic Potential Energy

• What is the potential energy of a spring compressed from equilibrium by a distance x?

Page 16: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Relating Force and Potential Energy

• Say we are given a Force as a function of position

• We can then write the change in potential energy associated with this (conservative) Force as:

Page 17: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Example

• Suppose we are given the potential energy as:

• What is the Force F as a function of x for this potential energy?

bxeAxxU 2)(

Page 18: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

3D Example

• In 3D

• So if

kzUj

yUi

xUzyxF ˆˆˆ),,(

xzxyzyxU 43),,(

Page 19: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Conservation of Energy

• For a conservative system (only conservative forces do work) where energy is transformed between kinetic and potential

• Work Energy Principle

• Relation between potential energy and work:

Page 20: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Conservation of Energy

• Combining the work-energy principle and our definition of potential energy, we see that:

• We can define the total mechanical energy of the system as:

• We can then see that the total energy of the system

• Is constant!

Page 21: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Conservation of Energy

• As long as no non-conservative forces do work, the total mechanical energy of the system is a conserved quantity!

• Principle of conservation of mechanical energy:– If only conservative forces are doing work, the total

mechanical energy of a system neither increases or decreases in any process. It is conserved.

Page 22: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Power of Energy Conservation

• Imagine dropping a mass m from a height h above the ground.

• Solve for speed of the mass at the ground using our equations of kinetic motion

Page 23: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Power of Energy Conservation• Imagine dropping a mass m from a height h

above the ground.• Now solve for speed of the mass at the ground

using energy conservation

Page 24: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Power of Energy Conservation

• But now, imagine sliding a mass m released from rest on the frictionless track shown below.

• Solve for speed of the mass at the ground using our equations of kinetic motion

h

Page 25: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Power of Energy Conservation

• But now, imagine sliding a mass m released from rest on the frictionless track shown below.

• Solve for speed of the mass at the ground using conservation of energy

h

Page 26: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Power of Energy Conservation

• We can even solve this if the mass is given an initial velocity vo.

• Solve for speed of the mass at the ground using conservation of energy

h

Page 27: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Example Problem• A 2 kg mass, starting at rest, slides down the frictionless

track shown below and into a spring with spring constant k=250N/m. How far is the spring compressed by the mass?

2m

Page 28: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Example Problem (Easier)• A 2 kg mass, starting at rest, slides down the frictionless

track shown below and into a spring with spring constant k=250N/m. How far is the spring compressed by the mass?

2m

Page 29: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Example Problem• A 2 kg mass, with an initial velocity of 5m/s, slides down

the frictionless track shown below and into a spring with spring constant k=250N/m. How far is the spring compressed by the mass?

2m

Page 30: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Spring Energy

• What is spring constant of catapult?• What is energy stored in spring?• what is Kinetic Energy of Watermelon?• What is velocity of watermelon?

• Assume– MassWoman=65kg– MassMelon=2kg– Δx=1.5m

Page 31: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Spring Energy

• What is spring constant of catapult?

1.5mθ=30°

Page 32: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Spring Energy• Need to know Force!• Free body diagram…

• With Force, we can now find k!

Page 33: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Spring Energy

• What is energy stored in spring?• What is Kinetic Energy of Watermelon?

Page 34: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

Spring Energy

• What is velocity of watermelon?• Assume

– MassMelon=2kg

Page 35: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

What does Energy vs Time look like?

US

K

E

Page 36: Physics I 95.141 LECTURE 13 10/20/10

Department of Physics and Applied Physics95.141, F2010, Lecture 13

What Did We Learn Today?

• Potential Energy

• Conservation of Mechanical Energy

• Concept of Energy Conservation is a powerful way to approach what might seem like complex problems!