Gravitational Potential Energy Function - Engineering Physics - Lecture Slides, Slides of Engineering Physics

Here you can find a complete lecture series on Engineering Physics course. These lecture slides includes: Gravitational Potential Energy Function, Total Energy, Radius, Repulsive Forces, Negative Total Energy, Bound States, Escape Velocity, Black Hole Radius

Typology: Slides

2013/2014

Uploaded on 01/31/2014

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Gravitational Potential Energy Function
U
=
โˆ’Gm
1
m
2
r
f
1,2
f
2,1
move together
v
v
docsity.com
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff
pf12
pf13
pf14
pf15
pf16
pf17

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Gravitational Potential Energy Function

U = โˆ’

Gm 1 m 2

r

f 1 ,^2

f 2 ,^1

move together

v

v

docsity.com

Gravitational Potential Energy Function

U = โˆ’

Gm 1 m 2

r

f 1 ,^2

f 2 ,^1

move together

v

v

U (^) g

0 r

Gravitational Potential Energy Function

U = โˆ’

Gm 1 m 2

r

f 1 ,^2

f 2 ,^1

rotate around

each other

v

v

Gravitational Potential Energy Function

U = โˆ’

Gm 1 m 2

r

f 1 ,^2

f 2 ,^1

rotate around

each other

v

Energy K+U is constant

U
K

r 0

Attraction: two stars

Clicker Quiz

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Consider a sattelite of mass m in orbit around a planet

of mass M at a radius r from the center of the planet.

What is the total energy of the sattelite?

  1. Etot = โˆ’

GmM

r

  1. Etot =

GmM

2 r

  1. Etot =

GmM

2 r^2

  1. Etot =

GmM

2 r^2

  1. Etot = โˆ’

GmM

2 r

Potential Energy Function Repulsive Forces

U =

q 1 q 2

r

Energy

K+U^ is constant

U

K

0

0

Repulsion: two protons

r โ†’ โˆž

Negative Total Energy

Negative Total Energy

Out of

K-energy

Clicker Quiz

Clicker Quiz

Bound States

Not enough

total energy

K + U < 0

K + U โ‰ฅ 0

Bound

Unbound

Application - Escape Velocity

Not enough

total energy

K + U < 0

K + U โ‰ฅ 0

Neglecting air resistance,

how fast must a projectile be fired to

escape from Earth's orbit?

Does it depend on:

t*OJUJBMLJOFUJDFOFSHZ

t.BTTPGQSPKFDUJMF

t.BTTPG&BSUI

Bound

Unbound

Application - Escape Velocity

vesc

  1. vf =

vrock โˆ’ vesc

  1. vf = vrock^2 + v^2 esc

  2. vf =

vrock + vesc

  1. vf = 2

vrock โˆ’ vesc

  1. vf = vrock^2 โˆ’ v^2 esc

Suppose the escape velocity from an asteroid is

If you throw a rock away from the asteroid at speed larger

than the escape velocity.

What is the final velocity of the rock?