units 17, 18, 19, 20 homework 3 is on the website of the course lazarian/ast103_2014

23
Units 17, 18, 19, 20 omework 3 is on the website of the course ://www.astro.wisc.edu/~lazarian/ast103_2014/

Upload: susanna-craig

Post on 18-Jan-2016

217 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Units 17, 18, 19, 20

Homework 3 is on the website of the coursehttp://www.astro.wisc.edu/~lazarian/ast103_2014/

Page 2: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Acceleration of a body is its rate of change of

A. MassB. Weight

C. VelocityD. Positions

Page 3: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

An object orbiting the sun in a circle can be said to be

A. WeightlessB. Always accelerating

C. Moving at a constant velocityD. Moving under equal and opposite forces

Page 4: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

An accelerating body must at all times

A. Have a changing direction of motionB. Have an increasing velocity

C. Be movingD. Have a changing velocity

Page 5: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Which of the following statements about an asteroid moving in a circular orbit around the Sun is untrue?

A. It is moving on a flat planeB. It is moving with constant velocity

C. It is acceleratingD. It is moving with constant speed

Page 6: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

• As we saw in Unit 17, we can find the mass of a large object by measuring the velocity of a smaller object orbiting it, and the distance between the two bodies.

• We can re-arrange this expression to get something very useful:

Orbits

G

VdM

2×=

dGM

Vcirc =We can use this expression to determinethe orbital velocity (V) of a small mass orbiting a distance d from the center of a much larger mass (M)

Page 7: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Calculating Escape Velocity

• From Newton’s laws of motion and gravity, we can calculate the velocity necessary for an object to have in order to escape from a planet, called the escape velocity

RGM

Vesc

2=

Page 8: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

What Escape Velocity Means

• If an object, say a rocket, is launched with a velocity less than the escape velocity, it will eventually return to Earth

• If the rocket achieves a speed higher than the escape velocity, it will leave the Earth, and will not return!

Page 9: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Escape Velocity is for more than just Rockets!

• The concept of escape velocity is useful for more than just rockets!

• It helps determine which planets have an atmosphere, and which don’t– Object with a smaller mass (such as the

Moon, or Mercury) have a low escape velocity. Gas particles near the planet can escape easily, so these bodies don’t have much of an atmosphere.

– Planets with a high mass, such as Jupiter, have very high escape velocities, so gas particles have a difficult time escaping. Massive planets tend to have thick atmospheres.

Page 10: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Konstantin Tsiolkovsky, pioneer of space exploration

Page 11: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Werner Von Braun --Dark Genius of Rocket Science

Page 12: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Centripetal Force

• If we tie a mass to a string and swing the mass around in a circle, some force is required to keep the mass from flying off in a straight line

• This is a centripetal force, a force directed towards the center of the system

• The tension in the string provides this force.

• Newton determined that this force can be described by the following equation:

d

VmFC

2×=

d

VmFC

2×=

Page 13: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

• We know that for planets, the centripetal force that keeps the planets moving on an elliptical path is the gravitational force.

• We can set FG and FC equal to each other, and solve for M!

• Now, if we know the orbital speed of a small object orbiting a much larger one, and we know the distance between the two objects, we can calculate the larger object’s mass!

Masses from Orbital Speeds

G

VdM

2×=

Page 14: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Newton’s Modification of Kepler’s 3rd Law

• Newton applied his ideas to Kepler’s 3rd Law, and developed a version that works for any two massive bodies, not just the Sun and its planets!

• Here, MA and MB are the two object’s masses expressed in units of the Sun’s mass.

• This expression is useful for calculating the mass of binary star systems, and other astronomical phenomena

2

3

YR

AUBA P

aMM =+

Page 15: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

The Origin of Tides

• The Moon exerts a gravitational force on the Earth, stretching it! – Water responds to

this pull by flowing towards the source of the force, creating tidal bulges both beneath the Moon and on the opposite side of the Earth

Page 16: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

High and Low Tides

As the Earth rotates beneath the Moon, the surface of the Earth experiences high and low tides

Page 17: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

The Sun creates tides, too!

• The Sun is much more massive than the Moon, so one might think it would create far larger tides!

• The Sun is much farther away, so its tidal forces are smaller, but still noticeable!

• When the Sun and the Moon line up, higher tides, call “spring tides” are formed

• When the Sun and the Moon are at right angles to each other, their tidal forces work against each other, and smaller “neap tides” result.

Page 18: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

The Conservation of Energy

• The energy in a closed system may change form, but the total amount of energy does not

change as a result of any process

Page 19: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

• Kinetic Energy is simply the energy of motion

• Both mass (m) and velocity (V) contribute to kinetic energy

• Imagine catching a thrown ball.– If the ball is thrown gently, it hits your hand

with very little pain

– If the ball is thrown very hard, it hurts to catch!

Kinetic Energy

2

2

1VmEK ×=

Page 20: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Thermal Energy

• Thermal energy is the energy associated with heat

• It is the energy of the random motion of individual atoms within an object.

• What you perceive as heat on a stovetop is the energy of the individual atoms in the heating element striking your finger

Page 21: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Potential Energy

• You can think of potential energy as stored energy, energy ready to be converted into another form

• Gravitational potential energy is the energy stored as a result of an object being lifted upwards against the pull of gravity

• Potential energy is released when the object is put into motion, or allowed to fall.

Page 22: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Definition of Angular Momentum

• Angular momentum is the rotational equivalent of inertia

• Can be expressed mathematically as the product of the objects mass, rotational velocity, and radius

• If no external forces are acting on an object, then its angular momentum is conserved, or a constant:

constant=××= rVmL

Page 23: Units 17, 18, 19, 20 Homework 3 is on the website of the course lazarian/ast103_2014

Conservation of Angular Momentum

• Since angular momentum is conserved, if either the mass, size or speed of a spinning object changes, the other values must change to maintain the same value of momentum– As a spinning figure skater

pulls her arms inward, she changes her value of r in angular momentum.

– Mass cannot increase, so her rotational speed must increase to maintain a constant angular momentum

• Works for stars, planets orbiting the Sun, and satellites orbiting the Earth, too!