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: F RAME -D MPLICATION - Gravity Probe B: Testing …einstein.stanford.edu/content/education/GP-B...

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A NEW UNDERSTANDING: CURVED SPACETIME In 1916, Einstein presented the world a new understand- ing of the universe: his General Theory of Relativity. In this theory, space is not an empty void, but an invisible struc- ture called “spacetime” . Nor is space simply a three- dimensional grid through which matter and light and energy move. It is a four-dimensional structure whose shape is curved and twisted by the presence of matter. What exactly is this “spacetime” that Einstein spoke of? For many, “spacetime” sounds like a science fiction concept where explorers travel through time on the way to parallel universes to meet alien life forms. In some ways, it is a simpler idea than that. The term “spacetime” simply refers to a frame of reference in which the three dimensions of space (x, y, z) and the dimension of time are used to describe motion or action in that frame of reference. Where spacetime gets interesting is when one considers that it is a frame of reference that is not always square. When a mass is present, such as a star or planet, the spacetime frame is deformed or curved by its presence. This means that the frame of reference, by which we measure the motion of things, is not a grid of straight lines and right angles but a grid that can be warped and curved. This idea contrasts directly with Newton’s concept of a fixed, immovable, universal grid upon which all motion can be measured. Take, for instance, the orbit of Mars around the Sun. From our perspective, it appears as though Mars is following a curved path through space. We think it is curved because we compare it with an invisible, fixed, square background. However, we can also imagine that Mars is following a straight path through space. It is a “straight” path because it is following the shape of spacetime. It just so happens that space itself is curved due to the presence of the Sun. HOW DOES CURVED SPACETIME EXPLAIN ORBITS? Our solar system is filled with objects following orbital paths. Planets orbit the Sun. Moons orbit the planets. Satellites and the International Space Station orbit the Earth. When Newton looked up at the night sky in the 17th century, he observed these orbital motions and concluded that, in accordance with his laws of motion, there must be a force acting on these objects to keep them in orbit. Why must there be a force? Because these objects were clearly moving in curved paths. Accord- ing to Newton’s law of inertia, the only way that an object would change direction from a straight path was if a force was acting on it. Since the planets and moons were constantly changing direc- tion (an orbit is an infinite series of turns), there must be a force constantly acting on them. Newton’s conclusion was that the force was “gravity” – an attractive force that emanated from each mass and pulled other masses in toward it. Einstein came to a different conclusion. From his perspective, the planets and moons in orbit in our solar system are not moving in curved paths. In fact, they are following straight lines through spacetime. It is spacetime that is curved, not the paths of the orbiting bodies. Since these bodies are not curving or turning, there is no force acting on them. No force is needed to explain these orbits; therefore, the attractive force of gravity does not exist. In fact, the orbiting masses are simply reacting to the shape of spacetime. How could the Earth, which so clearly seems to follow a curved path around the Sun, be said to be following a straight path? First, look closer at what “straight” means – it describes the motion of an object that stays parallel to a line in its frame of reference. Second, imagine that the grid lines on our frame of reference are curved. Around the Sun, the frame of reference is circular because the mass of the Sun has warped spacetime around it. Finally, trace the path of the Earth around the Sun. Notice that its path, while appearing curved at first, is actually moving parallel to the circular spacetime grid around Earth. The Earth is following a straight path around the Sun. This is how curved spacetime explains the orbital motion of all matter in the universe, from satel- lites to planets to binary stars to swirling galaxies, in addition to the Space Shuttle and the Interna- tional Space Station. The presence of a mass has an ability to curve local spacetime. As matter moves near the central mass, it follows this curve of spacetime. A SECOND IMPLICATION: FRAME-DRAGGING A few years after Einstein submitted his theory of curved spacetime, Austrian physicists Joseph Lense and Hans Thirring predicted that a mass could deform spacetime in a second way - through “frame-dragging” (1918). They proposed that the rotation of planets and stars or any rotating mass twists the spacetime frame near that mass. For example, not only is local spacet- ime curved near the Sun, it is twisted by the Sun’s rota- tion. Lense and Thirring predicted that this effect would be extremely small, and become smaller farther from the rotating mass, but it would occur around every rotating mass, be it a planet, a star, a galaxy, or a person. As yet, it is unclear how this phenomenon is supposed to occur, but the mathematical equations conclude that if masses curve spacetime, then they also must twist spa- cetime. DEMONSTRATION OF “F RAME-DRAGGINGThe purpose of this activity is to demonstrate how the Earth twists the local spacetime frame, but does not affect a distant spacetime frame. MATERIALS: Paper plate, honey, superball, food coloring, thumbtack, pushpin, peppercorn PROCEDURE: 1. Poke a tack through the center of the plate pointing upwards. 2. Pour a layer of honey on the plate. 2. Place the ball firmly on the tack. 3. Place a peppercorn in the honey near the edge of the plate. 4. Poke a pushpin in the top of the superball. 5. Squeeze a drop of food coloring in the honey around the ball. 5. Twist the superball as fast as you can. 6. Observe the effects of the twisting ball on the honey. QUESTIONS: 1. How does the honey react differently near the ball than far from the ball? 2. What do the parts of the model represent? The ball? The honey? The peppercorns? The food coloring? 3. What causes the “dragging” in the model? SUMMARY: The ball represents the Earth, the honey represents spacetime, and the peppercorn represents a distant mass (stars, planets, etc.) in spacetime. The food coloring is used to highlight the honey’s motion, and does not represent an astronomical object. The rotation of the Earth does twist the spacetime frame like the ball twists the honey, although it is not caused by “friction” between the Earth and local spacetime. The theory of gen - eral relativity states that spacetime and masses have a mysterious mutual “grip” on each other. EARTH WHITE DWARF (avg.) SIZE 12,756 km ~ 13,000 km MASS 6 x 10 24 kg ~ 1, 100,000 x 10 24 kg MODELS OF SPACETIME Using a plastic frame and spandex sheet, you can create a simple model of curved spacetime. On this model, you can demonstrate several phenomena that are caused by the curvature of spacetime. MATERIALS * Spandex sheet, 6’x 6’ -- (order from fabric store or web site) * PVC pipes and joints -- (cut to build a 5’x 5’x 3’ frame; complete instructions at http://einstein.stanford.edu/) * Large weights -- (bags of sand or water, iron/brass weight) * Small and large balls -- (superballs, steel/brass ball bearings, ping pong balls, golf balls, beach balls, etc.) A & B -- SATELLITE AND PLANETARY ORBITS 1. Place a heavy mass in the center of the sheet to create a sizable depression. 2. Pass out a small ball to each pair of students. Take turns to try out challenges. CHALLENGE A – You are sending a satellite to explore a distant planet behind a nearby planet. Stand on opposite sides of the center mass (the “near planet”). Roll the ball (your satellite) so that it reaches your partner (the “distant planet”) without hitting the center mass. CHALLENGE B – You want to put a satellite into orbit around the “near planet” . Work together and figure out how best to put your “satellite” into orbit around the center mass. C & D -- BENDING STARLIGHT & GRAVITATIONAL LENSEs 1. Place a heavy mass in the center of the sheet to create a sizable depression. Remind students that elec- tromagnetic waves (such as light) follow the curve of spacetime just like masses do. 2. Put students in groups of three. One person is a “star” emitting light in the form of a photon-ball. One person is an observer on Earth. The third person is the “marker” . CHALLENGE C - Demonstrate how starlight bends around large masses. Roll a ball from the “star” on one side of the sheet to the “Earth” on the other side of the sheet. The star and Earth should be directly opposite each other. The third person spots the point where the “photon-ball” turns towards the Earth. Once, she spots that point, she stands at the end of line coming from the Earth through the “turning point” . She is now the “apparent star.” CHALLENGE D – Demonstrate a gravitational lens. Have the “star” student roll two “photon-balls” around opposite sides of the central mass. Keep trying until both balls reach the “Earth” at the same time. Two students mark the “turning points” and stand in line with each point and the Earth. These students are two “apparent stars” created from the light of a single star. * Stars emit light in all directions, so starlight does not just go around one side of a central mass. If the star and the central mass are aligned properly, the star will appear on multiple sides of the central mass. It may appear as if there are several stars around the central mass. In fact, these stars are all part of the light coming from a single star. E -- BIGGER OBJECTS = GREATER GRAVITY? Which causes more curvature of spacetime (stronger gravity) -- the Earth or a white dwarf star? Even though they are the same size, the white dwarf is much more massive and creates a greater curvature of spacetime. Demonstrate the distinction with a whiffle ball and a baseball on the spandex sheet. The whiffle ball creates a much smaller depression or curve of spacetime than the baseball creates. Why? Because the baseball is more massive. In this case, mass matters, not size. EARTH STAR MODELS OF SPACETIME (CONT.) Questions A & B 1. What are the three key variables you must control when directing a satellite to where you want it to go? 2. Why is it impossible for you to put your “satellite” into perpetual orbit in this model, even though we do it in space all the time? C & D 3. Where does the star appear to be to the Earth-based observer? 4. Why is one star called an “apparent star”? 5. This phenomenon is called a “gravitational lens” . What does it have to do with gravity? 6. How is this phenomenon similar to what a lens does to light? E 7. What characteristic determines the amount of spacetime curvature or gravitational strength -- volume or mass? 8. What about the Sun and a neutron star? The Sun is about 100,000 times larger, but the neutron star has a little more mass. The Sun covers much more space; does this cause more curvature? 9. Do more dense objects always create more curvature than less dense objects? Answers -- #1 -- Initial speed, initial direction, distance of orbit from planet; #2 -- Friction between ball and sheet reduces speed causing ball to lose momentum; no friction in space so satellite’s momentum remains constant; #3 -- At the turning point, to the side of the central mass; #4 -- The star appears to be to the side of the central mass, but is actually behind the central mass; #5 -- The curvature of spacetime, which bends the starlight, is referred to as gravity; #6 -- Just like a lens, the curvature of spacetime around the central mass bends incoming light and focuses it to a common point; #7 -- Mass determines curvature or gravitational strength; #8 -- Even though the Sun covers more space, the more massive object always creates more curvature or gravity; #9 -- No. A denser object may not have as much mass as a less dense object. Compare a steel ship and a quarter. The ship is less dense (it floats), but has more overall mass. James Overduin, Pancho and Evelyn Eekels, and Kate Stephenson
Transcript

A N

EW U

ND

ERST

AN

DIN

G: C

UR

VED

SPA

CET

IME

In 1

916,

Ein

stei

n p

rese

nte

d t

he

wo

rld

a n

ew u

nd

erst

and

-in

g o

f th

e u

niv

erse

: his

Gen

eral

Th

eory

of R

elat

ivit

y. I

n t

his

th

eory

, sp

ace

is n

ot

an e

mp

ty v

oid

, bu

t an

invi

sib

le s

tru

c-tu

re

calle

d “

spac

etim

e”.

No

r is

sp

ace

sim

ply

a

thre

e-d

imen

sio

nal

gri

d t

hro

ug

h w

hic

h m

atte

r an

d l

igh

t an

d

ener

gy

mov

e. I

t is

a f

ou

r-d

imen

sio

nal

str

uct

ure

wh

ose

sh

ape

is c

urv

ed a

nd

tw

iste

d b

y th

e p

rese

nce

of m

atte

r.

Wh

at e

xact

ly is

th

is “s

pac

etim

e” t

hat

Ein

stei

n s

po

ke o

f?

For

man

y, “s

pac

etim

e” s

ou

nd

s lik

e a

scie

nce

fic

tio

n c

on

cep

t w

her

e ex

plo

rers

tra

vel t

hro

ug

h t

ime

on

the

way

to p

aral

lel u

niv

erse

s to

mee

t alie

n li

fe fo

rms.

In s

om

e w

ays,

it is

a s

imp

ler i

dea

than

that

. Th

e te

rm “s

pac

etim

e” s

imp

ly re

fers

to a

fram

e o

f ref

eren

ce in

wh

ich

the

thre

e d

imen

sio

ns

of s

pac

e (x

, y, z

) an

d t

he

dim

ensi

on

of t

ime

are

use

d to

des

crib

e m

oti

on

or a

ctio

n in

th

at fr

ame

of r

efer

ence

.

Wh

ere

spac

etim

e g

ets

inte

rest

ing

is w

hen

on

e co

nsi

der

s th

at it

is a

fram

e o

f ref

eren

ce t

hat

is n

ot

alw

ays

squ

are.

Wh

en a

mas

s is

pre

sen

t, su

ch a

s a

star

or

pla

net

, th

e sp

acet

ime

fram

e is

def

orm

ed

or

curv

ed b

y it

s p

rese

nce

. Th

is m

ean

s th

at t

he

fram

e o

f re

fere

nce

, by

wh

ich

we

mea

sure

th

e m

oti

on

of t

hin

gs,

is n

ot

a g

rid

of s

trai

gh

t lin

es a

nd

rig

ht

ang

les

bu

t a

gri

d t

hat

can

be

war

ped

an

d

curv

ed.

This

idea

co

ntr

asts

dir

ectl

y w

ith

New

ton’

s co

nce

pt

of

a fix

ed, i

mm

ovab

le, u

niv

ersa

l gri

d

up

on

wh

ich

all

mo

tio

n c

an b

e m

easu

red

.

Take

, fo

r in

stan

ce, t

he

orb

it o

f M

ars

aro

un

d t

he

Sun

. Fr

om

ou

r p

ersp

ecti

ve, i

t ap

pea

rs a

s th

ou

gh

Mar

s is

fo

llow

ing

a c

urv

ed p

ath

th

rou

gh

sp

ace.

We

thin

k it

is

curv

ed b

ecau

se w

e co

mp

are

it w

ith

an

invi

sib

le, f

ixed

, sq

uar

e b

ackg

rou

nd

.

Ho

wev

er, w

e ca

n a

lso

imag

ine

that

Mar

s is

follo

win

g a

str

aig

ht p

ath

thro

ug

h s

pac

e. I

t is

a “s

trai

gh

t”

pat

h b

ecau

se it

is fo

llow

ing

th

e sh

ape

of s

pac

etim

e. I

t ju

st s

o h

app

ens

that

sp

ace

itse

lf is

cu

rved

d

ue

to t

he

pre

sen

ce o

f th

e Su

n.

HO

W D

OES

CU

RV

ED S

PAC

ETIM

E EX

PLA

IN O

RB

ITS?

Ou

r so

lar

syst

em is

fille

d w

ith

ob

ject

s fo

llow

ing

orb

ital

pat

hs.

Pla

net

s o

rbit

th

e Su

n. M

oo

ns

orb

it

the

pla

net

s. S

atel

lites

an

d t

he

Inte

rnat

ion

al S

pac

e St

atio

n o

rbit

th

e Ea

rth

. W

hen

New

ton

loo

ked

u

p a

t th

e n

igh

t sk

y in

th

e 17

th c

entu

ry, h

e o

bse

rved

th

ese

orb

ital

mo

tio

ns

and

co

ncl

ud

ed t

hat

, in

ac

cord

ance

wit

h h

is la

ws

of m

oti

on

, th

ere

mu

st b

e a

forc

e ac

tin

g o

n th

ese

ob

ject

s to

kee

p th

em in

o

rbit

.

Wh

y m

ust

th

ere

be

a fo

rce?

Bec

ause

th

ese

ob

ject

s w

ere

clea

rly

mov

ing

in c

urv

ed p

ath

s. A

cco

rd-

ing

to N

ewto

n’s

law

of i

ner

tia,

th

e o

nly

way

th

at a

n o

bje

ct w

ou

ld c

han

ge

dir

ecti

on

fro

m a

str

aig

ht

pat

h w

as if

a fo

rce

was

act

ing

on

it. S

ince

the

pla

net

s an

d m

oo

ns

wer

e co

nst

antl

y ch

ang

ing

dir

ec-

tio

n (

an o

rbit

is

an i

nfin

ite

seri

es o

f tu

rns)

, th

ere

mu

st b

e a

forc

e co

nst

antl

y ac

tin

g o

n t

hem

. N

ewto

n’s

con

clu

sio

n w

as th

at th

e fo

rce

was

“gra

vity

” – a

n a

ttra

ctiv

e fo

rce

that

em

anat

ed fr

om

eac

h

mas

s an

d p

ulle

d o

ther

mas

ses

in to

war

d it

.

Ein

stei

n c

ame

to a

diff

eren

t co

ncl

usi

on

. Fr

om

his

per

spec

tive

, th

e p

lan

ets

and

mo

on

s in

orb

it in

o

ur s

ola

r sys

tem

are

no

t m

ovin

g in

cu

rved

pat

hs.

In fa

ct, t

hey

are

follo

win

g s

trai

gh

t lin

es t

hro

ug

h

spac

etim

e. I

t is

sp

acet

ime

that

is c

urv

ed, n

ot

the

pat

hs

of t

he

orb

itin

g b

od

ies.

Sin

ce t

hes

e b

od

ies

are

no

t cu

rvin

g o

r tu

rnin

g, t

her

e is

no

forc

e ac

tin

g o

n t

hem

. N

o fo

rce

is n

eed

ed t

o e

xpla

in t

hes

e o

rbit

s; t

her

efo

re, t

he

attr

acti

ve f

orc

e o

f g

ravi

ty d

oes

no

t ex

ist.

In

fac

t, th

e o

rbit

ing

mas

ses

are

sim

ply

reac

tin

g to

th

e sh

ape

of s

pac

etim

e.

Ho

w c

ou

ld th

e Ea

rth

, wh

ich

so

cle

arly

see

ms

to fo

llow

a c

urv

ed p

ath

aro

un

d th

e Su

n, b

e sa

id to

be

follo

win

g a

str

aig

ht p

ath

? F

irst

, lo

ok

clo

ser a

t wh

at “s

trai

gh

t” m

ean

s –

it d

escr

ibes

the

mo

tio

n o

f an

o

bje

ct t

hat

sta

ys p

aral

lel t

o a

lin

e in

its

fram

e o

f ref

eren

ce.

Seco

nd,

imag

ine

that

th

e g

rid

lin

es o

n

ou

r fr

ame

of r

efer

ence

are

cu

rved

. A

rou

nd

th

e Su

n, t

he

fram

e o

f ref

eren

ce is

cir

cula

r b

ecau

se t

he

mas

s o

f th

e Su

n h

as w

arp

ed s

pac

etim

e ar

ou

nd

it.

Fin

ally

, tra

ce t

he

pat

h o

f th

e Ea

rth

aro

un

d t

he

Sun

. N

oti

ce t

hat

its

pat

h, w

hile

ap

pea

rin

g c

urv

ed a

t fir

st, i

s ac

tual

ly m

ovin

g p

aral

lel t

o t

he

circ

ula

r sp

acet

ime

gri

d a

rou

nd

Ear

th. T

he

Eart

h is

follo

win

g a

str

aig

ht

pat

h a

rou

nd

th

e Su

n.

This

is h

ow

cu

rved

sp

acet

ime

exp

lain

s th

e o

rbit

al m

oti

on

of a

ll m

atte

r in

th

e u

niv

erse

, fro

m s

atel

-lit

es to

pla

net

s to

bin

ary

star

s to

sw

irlin

g g

alax

ies,

in a

dd

itio

n to

the

Spac

e Sh

utt

le a

nd

the

Inte

rna-

tio

nal

Sp

ace

Stat

ion

. Th

e p

rese

nce

of

a m

ass

has

an

ab

ility

to

cu

rve

loca

l sp

acet

ime.

A

s m

atte

r m

oves

nea

r th

e ce

ntr

al m

ass,

it fo

llow

s th

is c

urv

e o

f sp

acet

ime.

A S

ECO

ND

IMP

LIC

ATI

ON

: FR

AM

E-D

RA

GG

ING

A f

ew y

ears

aft

er E

inst

ein

su

bm

itte

d h

is t

heo

ry o

f cu

rved

sp

acet

ime,

Au

stri

an p

hys

icis

ts J

ose

ph

Len

se

and

Han

s Th

irri

ng

pre

dic

ted

that

a m

ass

cou

ld d

efo

rm

spac

etim

e in

a s

eco

nd

way

- th

rou

gh

“fra

me-

dra

gg

ing”

(1

918)

. Th

ey p

rop

ose

d th

at th

e ro

tati

on

of p

lan

ets

and

st

ars

or

any

rota

tin

g m

ass

twis

ts t

he

spac

etim

e fr

ame

nea

r th

at m

ass.

Fo

r ex

amp

le, n

ot

on

ly is

loca

l sp

acet

-im

e cu

rved

nea

r th

e Su

n, i

t is

twis

ted

by

the

Sun’

s ro

ta-

tio

n.

Len

se a

nd

Th

irri

ng

pre

dic

ted

th

at t

his

eff

ect

wo

uld

be

extr

emel

y sm

all,

and

bec

om

e sm

alle

r fa

rth

er fr

om

the

rota

tin

g m

ass,

bu

t it w

ou

ld o

ccu

r aro

un

d e

very

rota

tin

g m

ass,

be

it a

pla

net

, a s

tar,

a g

alax

y, o

r a

per

son

. A

s ye

t, it

is

un

clea

r h

ow

th

is p

hen

om

eno

n i

s su

pp

ose

d t

o o

ccu

r, b

ut

the

mat

hem

atic

al e

qu

atio

ns

con

clu

de

that

if m

asse

s cu

rve

spac

etim

e, t

hen

th

ey a

lso

mu

st t

wis

t sp

a-ce

tim

e.

DEM

ON

STR

ATI

ON

OF “

FR

AM

E-D

RA

GG

ING

” Th

e p

urp

ose

of t

his

act

ivit

y is

to d

emo

nst

rate

ho

w t

he

Eart

h t

wis

ts t

he

loca

l sp

acet

ime

fram

e, b

ut

do

es n

ot

affe

ct a

dis

tan

t sp

acet

ime

fram

e.

M

ATE

RIA

LS: P

aper

pla

te, h

on

ey, s

up

erb

all,

foo

d c

olo

rin

g, t

hu

mb

tack

, pu

shp

in, p

epp

erco

rn

P

RO

CED

UR

E:

1. P

oke

a t

ack

thro

ug

h t

he

cen

ter o

f th

e p

late

po

inti

ng

up

war

ds.

2. P

ou

r a la

yer o

f ho

ney

on

th

e p

late

. 2.

Pla

ce t

he

bal

l fir

mly

on

th

e ta

ck.

3. P

lace

a p

epp

erco

rn in

th

e h

on

ey n

ear t

he

edg

e o

f th

e p

late

. 4.

Po

ke a

pu

shp

in in

th

e to

p o

f th

e su

per

bal

l. 5.

Sq

uee

ze a

dro

p o

f fo

od

co

lori

ng

in t

he

ho

ney

aro

un

d t

he

bal

l. 5.

Tw

ist

the

sup

erb

all a

s fa

st a

s yo

u c

an.

6. O

bse

rve

the

effe

cts

of t

he

twis

tin

g b

all o

n t

he

ho

ney

.

QU

ESTI

ON

S: 1.

How

doe

s th

e ho

ney

reac

t diff

eren

tly

near

the

ball

than

far f

rom

the

ball?

2.

Wha

t do

the

part

s of

the

mod

el re

pres

ent?

The

bal

l? T

he h

oney

? T

he p

eppe

rcor

ns?

The

food

col

orin

g?

3. W

hat c

ause

s th

e “d

ragg

ing”

in th

e m

odel

?

SUM

MA

RY:

The

bal

l rep

rese

nts

the

Eart

h, t

he

ho

ney

rep

rese

nts

sp

acet

ime,

an

d th

e p

epp

erco

rn re

pre

sen

ts a

dis

tan

t mas

s

(sta

rs, p

lan

ets,

etc.

) in

sp

acet

ime.

Th

e fo

od

co

lori

ng

is u

sed

to

hig

hlig

ht

the

ho

ney

’s m

oti

on

, an

d d

oes

no

t re

pre

sen

t an

ast

ron

om

ical

ob

ject

. Th

e ro

tati

on

of t

he

Eart

h d

oes

twis

t th

e sp

acet

ime

fram

e lik

e th

e b

all t

wis

ts

the

ho

ney

, alt

ho

ug

h it

is n

ot

cau

sed

by

“fri

ctio

n” b

etw

een

th

e Ea

rth

an

d lo

cal s

pac

etim

e. T

he

theo

ry o

f gen

-er

al re

lati

vity

sta

tes

that

sp

acet

ime

and

mas

ses

hav

e a

mys

teri

ou

s m

utu

al “g

rip”

on

eac

h o

ther

.

EA

RTH

WH

ITE

DW

ARF

(avg

.)

SIZ

E

1

2,75

6 km

~

13,

000

km

MA

SS

6

x 10

24 k

g

~ 1

, 100

,000

x 1

024 k

g

MO

DEL

S O

F SP

AC

ETIM

E U

sin

g a

pla

stic

fram

e an

d s

pan

dex

sh

eet,

you

can

cre

ate

a si

mp

le m

od

el o

f cu

rved

sp

acet

ime.

On

th

is m

od

el, y

ou

can

dem

on

stra

te s

ever

al p

hen

om

ena

that

ar

e ca

use

d b

y th

e cu

rvat

ure

of s

pac

etim

e.

MAT

ERIA

LS

* Sp

and

ex s

hee

t, 6’

x 6’

--

(ord

er fr

om fa

bric

sto

re o

r web

site

) *

PVC

pip

es a

nd

join

ts -

- (c

ut to

bui

ld a

5’x

5’x

3’ f

ram

e; c

ompl

ete

inst

ruct

ions

at h

ttp:

//ei

nste

in.s

tanf

ord.

edu/

) *

Larg

e w

eig

hts

--

(bag

s of

san

d or

wat

er, i

ron/

bras

s w

eigh

t)

* Sm

all a

nd

larg

e b

alls

--

(sup

erba

lls, s

teel

/bra

ss b

all b

eari

ngs,

ping

pon

g ba

lls, g

olf b

alls

, bea

ch b

alls

, etc

.) A

& B

-- S

ATE

LLIT

E A

ND

PLA

NET

AR

Y O

RB

ITS

1. P

lace

a h

eavy

mas

s in

th

e ce

nte

r of t

he

shee

t to

cre

ate

a si

zab

le d

epre

ssio

n.

2. P

ass

ou

t a

smal

l bal

l to

eac

h p

air o

f stu

den

ts. T

ake

turn

s to

try

ou

t ch

alle

ng

es.

CH

ALL

ENG

E A

– Y

ou

are

sen

din

g a

sat

ellit

e to

exp

lore

a d

ista

nt

pla

net

b

ehin

d a

nea

rby

pla

net

. St

and

on

op

po

site

sid

es o

f th

e ce

nte

r mas

s

(th

e “n

ear p

lan

et”)

. R

oll

the

bal

l (yo

ur s

atel

lite)

so

th

at it

reac

hes

yo

ur p

artn

er (t

he

“dis

tan

t p

lan

et”)

wit

ho

ut

hit

tin

g t

he

cen

ter m

ass.

CH

ALL

ENG

E B

– Y

ou

wan

t to

pu

t a

sate

llite

into

orb

it a

rou

nd

th

e “n

ear p

lan

et”.

Wo

rk to

get

her

an

d fi

gu

re o

ut

ho

w b

est

to

pu

t yo

ur “

sate

llite

” in

to o

rbit

aro

un

d t

he

cen

ter m

ass.

C &

D --

BEN

DIN

G S

TAR

LIG

HT

& G

RA

VIT

ATI

ON

AL

LEN

SEs

1. P

lace

a h

eavy

mas

s in

th

e ce

nte

r o

f th

e sh

eet

to c

reat

e a

siza

ble

dep

ress

ion

. R

emin

d s

tud

ents

th

at e

lec-

tro

mag

net

ic w

aves

(su

ch a

s lig

ht)

follo

w t

he

curv

e o

f sp

acet

ime

just

like

mas

ses

do.

2.

Pu

t st

ud

ents

in g

rou

ps

of

thre

e. O

ne

per

son

is a

“sta

r” e

mit

tin

g li

gh

t in

th

e fo

rm o

f a

ph

oto

n-b

all.

On

e p

erso

n is

an

ob

serv

er o

n E

arth

. T

he

thir

d p

erso

n is

th

e “m

arke

r”.

CH

ALL

ENG

E C

- D

emo

nst

rate

ho

w s

tarl

igh

t b

end

s ar

ou

nd

larg

e m

asse

s. R

oll

a b

all f

rom

th

e “s

tar”

on

on

e si

de

of t

he

shee

t to

the

“Ear

th” o

n th

e o

ther

sid

e o

f th

e sh

eet.

Th

e st

ar a

nd

Ear

th s

ho

uld

be

dir

ectl

y o

pp

osi

te

each

oth

er.

The

thir

d p

erso

n s

po

ts t

he

po

int

wh

ere

the

“ph

oto

n-b

all”

turn

s to

war

ds

the

Eart

h.

On

ce,

she

spo

ts t

hat

po

int,

she

stan

ds

at t

he

end

of l

ine

com

ing

fro

m t

he

Eart

h t

hro

ug

h t

he

“tu

rnin

g p

oin

t”.

She

is n

ow

th

e “a

pp

aren

t st

ar.”

CH

ALL

ENG

E D

– D

emo

nst

rate

a g

ravi

tati

on

al l

ens.

Hav

e th

e “s

tar”

stu

den

t ro

ll tw

o “p

ho

ton

-bal

ls”

aro

un

d

op

po

site

sid

es o

f th

e ce

ntr

al m

ass.

Kee

p tr

yin

g u

nti

l bo

th b

alls

reac

h th

e “E

arth

” at

the

sam

e ti

me.

Tw

o

stu

den

ts m

ark

the

“tu

rnin

g p

oin

ts” a

nd

sta

nd

in li

ne

wit

h e

ach

po

int a

nd

the

Eart

h. T

hes

e st

ud

ents

are

tw

o “a

pp

aren

t st

ars”

cre

ated

fro

m t

he

ligh

t o

f a s

ing

le s

tar.

* S

tars

em

it li

gh

t in

all

dir

ecti

on

s, so

sta

rlig

ht d

oes

no

t ju

st g

o a

rou

nd

on

e si

de

of a

cen

tral

mas

s. If

the

star

an

d th

e ce

ntr

al m

ass

are

alig

ned

pro

per

ly, t

he

star

will

ap

pea

r on

mu

ltip

le s

ides

of t

he

cen

tral

mas

s.

It m

ay a

pp

ear a

s if

ther

e ar

e se

vera

l sta

rs a

rou

nd

the

cen

tral

mas

s. In

fact

, th

ese

star

s ar

e al

l par

t of t

he

ligh

t co

min

g fr

om

a s

ing

le s

tar.

E --

BIG

GER

OB

JEC

TS =

GR

EATE

R G

RA

VIT

Y?

Wh

ich

cau

ses

mo

re c

urv

atu

re o

f sp

acet

ime

(str

on

ger

gra

vity

) -- t

he

Eart

h o

r a w

hit

e d

war

f sta

r?

Even

th

ou

gh

th

ey a

re t

he

sam

e si

ze, t

he

wh

ite

dw

arf i

s m

uch

m

ore

mas

sive

an

d c

reat

es a

gre

ater

cu

rvat

ure

of

spac

etim

e.

Dem

on

stra

te th

e d

isti

nct

ion

wit

h a

wh

iffle

bal

l an

d a

bas

ebal

l o

n th

e sp

and

ex s

hee

t. T

he

wh

iffle

bal

l cre

ates

a m

uch

sm

alle

r d

epre

ssio

n o

r cu

rve

of s

pac

etim

e th

an t

he

bas

ebal

l cre

ates

.

Wh

y? B

ecau

se t

he

bas

ebal

l is

mo

re m

assi

ve.

In t

his

cas

e, m

ass

mat

ters

, no

t si

ze.

EART

H

STA

R

MO

DEL

S OF S

PACE

TIM

E (CO

NT.

) Q

uest

ions

A

& B

1.

Wha

t are

the

thre

e ke

y va

riabl

es y

ou m

ust c

ontr

ol w

hen

dire

ctin

g a

sate

llite

to w

here

you

wan

t it t

o go

? 2.

Why

is it

impo

ssib

le fo

r you

to p

ut y

our “

sate

llite

” int

o pe

rpet

ual o

rbit

in th

is m

odel

, eve

n th

ough

we

do it

in s

pace

all

the

time?

C

& D

3.

Whe

re d

oes t

he st

ar a

ppea

r to

be to

the

Eart

h-ba

sed

obse

rver

?

4. W

hy is

one

star

calle

d an

“app

aren

t sta

r”?

5. T

his p

heno

men

on is

calle

d a

“gra

vita

tiona

l len

s”. W

hat d

oes i

t hav

e to

do

with

gra

vity

?

6. H

ow is

this

phe

nom

enon

sim

ilar t

o w

hat a

lens

doe

s to

light

? E

7. W

hat c

hara

cter

istic

det

erm

ines

the

amou

nt o

f spa

cetim

e cu

rvat

ure

or g

ravi

tatio

nal s

tren

gth

-- v

olum

e or

mas

s?

8. W

hat a

bout

the

Sun

and

a ne

utro

n st

ar?

The

Sun

is a

bout

100

,000

tim

es la

rger

, but

the

neut

ron

star

has

a li

ttle

mor

e m

ass.

Th

e Su

n co

vers

muc

h m

ore

spac

e; d

oes t

his c

ause

mor

e cu

rvat

ure?

9.

Do

mor

e de

nse

obje

cts a

lway

s cre

ate

mor

e cu

rvat

ure

than

less

den

se o

bjec

ts?

Answ

ers -- #1 -- Initial speed, initial direction, distance of orbit from planet; #2 -- Friction betw

een ball and sheet reduces speed causing ball to lose m

omentum

; no friction in space so satellite’s mom

entum rem

ains constant; #3 -- At the turning point, to the side of the central m

ass; #4 -- The star appears to be to the side of the central m

ass, but is actually behind the central mass; #5 -- The curvature of spacetim

e, which bends the starlight, is

referred to as gravity; #6 -- Just like a lens, the curvature of spacetime around the central m

ass bends incoming light and focuses it to a com

mon

point; #7 -- Mass determ

ines curvature or gravitational strength; #8 -- Even though the Sun covers more space, the m

ore massive object alw

ays creates m

ore curvature or gravity; #9 -- No. A

denser object may not have as m

uch mass as a less dense object. C

ompare a steel ship and a quarter.

The ship is less dense (it floats), but has more overall m

ass.

James Overduin, Pancho and Evelyn Eekels, and Kate Stephenson

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