...was born in Pisa, Italy on February 15, 1564. His family were of nobility but not rich.
In 1581, Galileo began studies at the University of Pisa, where he learned Aristotelian physics which held that heavier objects fall faster through a medium than lighter ones. Galileo eventually disproved this idea and asserted that all objects, regardless of density, fall at the same rate in a vacuum. To determine this rate, Galileo performed various experiments with dropped objects from a certain height. In an early experiment, he rolled balls down a gently inclined plane; then, he determined their positions after equal time intervals. He wrote down his discoveries about motion in his book, De Motu, "On Motion." |
DISTANCE TRAVELED
| d = t × VAve |
Elapsed
Time | Final
Speed | Ave.
Speed | Total
Dist. |
| t | VFin | VAve | d |
| 1 sec | 10 m/s | 5 m/s | 5 m |
| 2 sec | 20 m/s | 10 m/s | 20 m |
| 3 sec | 30 m/s | 15 m/s | 45 m |
| . . . | ... | ... | ... |
| 10 sec | 100 m/s | 50 m/s | 500 m |
| Given | g × t | Vfin/2 | t × Vave |
| g×t | g×t/2 | g×t2/2 |
Gravity accelerates freely falling objects 10 meters per second for every second of flight. After 3 sec, object's speed is 30 m/sec. However, the distance fallen will reflect object's average speed. For example, it falls 5 meters in first second of free fall due to its average speed of 5 meters per second.
After three seconds, the object achieves an average speed (VAve) of 15 meters per second; multiplying this value by 3 seconds duration gives us 45 meters distance. |
ALTERNATE DISTANCE METHOD
Since 10m=.01km, let g ≈ .01 km/sec2
| t | t2 | d |
Time
(sec) | | Distance
(km) |
10
|
100
|
.5
|
60
|
3,600
|
18
|
3,600
|
1.296×106
|
64,800
|
86,400
|
7.464×109
|
37,324,800
|
t
|
t2
|
g × t2 /2
|
Determine distance traveled with another simple equation.
Recall: VAve = VFin/2
Thus, d= V Ave × t = t(V Fin/2).
Recall: VFin = a × t
d = t(VFin/2) = t (a × t/2)
d = (a × t2)/2.
Use a = g = .01 km/sec2;
then, g-force distances can be determined:
d = g × t2/2
Final data row uses elapsed time for an entire day (86,400 sec); thus, g-force distance is for an entire day. (Recall that one Astronomical Unit (AU), average distance from Sol to Terra, is about 150 million km. Thus, traveling at g-force for one day takes us about 1/4 AU. See below for more details.) |
GALILEO'S MOST FAMOUS INVENTION
... was the telescope. In 1609, Galileo’s first telescope was modeled after previous telescopes that could magnify images three times. He soon created another telescope which could magnify twenty times.
 With this improved telescope, he could observe features on the moon, observe a supernova, verify the phases of Venus, discover sunspots and discover the four largest satellites of Jupiter.
His discoveries confirmed the Copernican system; Earth and other planets revolve around the Sun. This starkly contrasted with the view of the Church which then held the Universe to be geocentric.
Galileo's belief in the Copernican System eventually got him into trouble with the Catholic Church’s Inquisition which was charged with the eradication of heresies. A Church committee of consultants declared this Copernican proposition to be heretical. Because Galileo supported the Copernican system, he was warned to not discuss or defend Copernican theories. |
GALILEO FACES THE INQUISITION In 1624, Galileo understood from Pope Urban VIII that he could write about Copernican theory as long as he treated it as a mathematical proposition; thus, he felt safe to publish Dialogue Concerning the Two Chief World Systems. However, certain mean spirited enemies of Galileo persuaded the Pope to interpret certain passages as personal insults. Thus, Galileo was called to Rome in 1633 to face the Inquisition. Galileo was found guilty of heresy for his Dialogue …, and was sent to his home near Florence to be under house arrest for the rest of his life. Though disappointed by the verdict, this distraction free environment enabled Galileo to produce yet more scientific work. In 1642, Galileo died at his home. Isaac Newton was born the same year. |
kilometers per second (kps) per day
Express g differently
| g | = | 10 m
sec2 | × | 1 km
1000 m |
| g | = | .01 kps
sec | × | 86,400 sec
day |
| g | = | 864 kps
day | | |
After 86,400 seconds (one day) of g-force acceleration, final velocity is 864 km per second:
Vfin = g × t = 864 km/sec
For every day of constant acceleration, g; spacecraft increases its velocity another 864 km/sec. Thus, we can restate g as a daily rate.
g = 864 km per sec / day
Thus, at end of 2nd day of spaceflight,
| VFin = t × 864 kps/day |
Elapsed
Time (t) | Final
Vel. (VFin) |
| days | kps |
1
|
864
|
2
|
1,728
|
3 | 2,592
|
..
|
......
|
10 | 8,640
|
| Given | g × t |
Vfin = g × t
Vfin = 864 km/sec /day × 2 days
Vfin = 1,728 km/sec
Table shows additional values.
Why express g as "kps/day"? Quickly determine inflight velocities as kilometers per second (kps), which is typically used for orbital velocities of Solar System objects (planets, asteroids, comets). For example, Earth's orbital velocity around Sol is about 30 kps. NOTE: After just one day of g-force acceleration, spacecraft attains tremendous speed many times this.
|
|
Astronomical Units (AUs)/day per day
Thought Experiment (TE) considers the Astronomical Unit (AU), average distance from Earth to Sol. Distance to nearby planets is conveniently measured in AUs.
Exact AU = 149,597,870 km; for convenience, TE rounds AU to 150,000,000 km.
Express g differently
| g | = | 864 kps
day | × | 86,400 sec
day |
| g | = | 74,649,600 km
day2 | × | 1 AU
149,597,870 km |
| g | ≈ | .5 AU
day2 |
g ≈ .5 AU/day2
Different g expression enables different velocity expressions.
After one day of g-force acceleration:
VFin = t × g
VFin = 1 day × .5 AU/day2
VFin = .5 AU/day
VAve = VFin /2
VAve = .5 AU/day ÷ 2
VAve = .25 AU/day
|
Elapsed
Time (t) | Final Vel. (VFin) | Ave Vel. (VAve) | Ttl Dist. (d) |
| day | AU/day | AU/day | AU |
1
|
.5
|
.25
|
.25
|
2
|
1.0
|
.5
|
1.0
|
3
|
1.5
|
.75
|
2.25
|
. . .
|
...
|
...
|
...
|
10
|
5.0
|
2.5
|
25
|
| Given | g × t | VFin/2 | t × VAve |
| g×t | g×t/2 | g×t2/2 |
Interplanetary g-force flights will be quick, a matter of days.
Therefore,
g ≈ 0.5 AU/day2 might be a
convenient expression. |
Galileo showed that the free-fall motion of an object has a constant acceleration. Starting from rest, distances increase in proportion to the square of the elapsed time.
Since a vertical fall was too fast for Galileo to measure accurately, he slowed it down by making the ball roll down an inclined board. Across the board, along to its surface, he strung a number of taut horizontal wires, making the ball sound a click whenever it jumped over one of them. Galileo then moved the wires up and down the board, until the clicks sounded evenly spaced.
The board's slope slows ball's velocity to much less than free fall, but Earth's gravity still pulling it downward. The time, t, is measured by the audible clicks. Starting with the ball at rest (D0 = 0), one measures following:
After one click,
|
D1 = 1
|
unit
|
After two clicks,
|
D2= 4
|
units
|
After three clicks,
|
D3= 9
|
units
|
After x clicks,
| Dx= x2 | units |
Galileo confirmed the ratio between the distances to be that of the squares: 1, 4, 9, 16, 25… If one converts clicks into seconds and accounts for the angle of the board as well as for the rolling friction of the ball (not available in Galileo's day), one could even calculate Earth's gravity, g, from observed acceleration, a.
For more on this experiment, see the book "The God Particle" by Nobel prize winner, Leon Lederman, with Dick Teresi.
|
Percent Light Speed (%c) per day
Finally, consider g in terms of %c, percent light speed.
Express light speed, c, differently
| c | = | 299,792.458 km
sec | × | 86,400 sec
day |
| c | = | 299,792.5×86,400km
day | × | 1 AU
149,597,870km |
| c | ≈ | 173.145 AU
day |
First, convert c from the well known kilometers per second to AUs per day.
Express g in terms of c
| g | ≈ | 10 m
sec × sec | = | .5 AU
day × day |
| g | ≈ | .5 AU/day
day | × | c
173.145 AU/day |
| g | ≈ | .00289 c
day | = | .289% c
day |
Recall that g-force acceleration equals 0.5 AU/day; thus, we can readily transform this value into a percentage of light speed.
Recall that %c is a velocity, and g is an acceleration (velocity per unit time); thus, another value for g is 0.289%c/day.
Do we care about our spacecraft's light speed??
Relativistic effects might be a concern for very fast inflight speeds. |
RELATIVISTIC EFFECTS
| VFin = t × .289%c/day |
Elapsed
Time (t) | Final Vel. (VFin) |
| day | %c |
| 1 | 0.289 |
| 2 | 0.578 |
| 3 | 0.867 |
| .. | ...... |
| 10 | 2.890 |
| Given | g × t |
| 1. For interplanetary flights, we don't care about relativistic effects.
Even at g-force acceleration, ship's speed never exceeds 10% c throughout the Solar System.
Such flights will take a few days, and table shows that we don't even reach 1% c until after three days of g-force flight.
NOTE: Due to relativistic effects, our g-force spaceship will never ever reach light speed, c; even though, it can get ever closer and closer. Thus, short time measures of g-force accelerated velocities can be approximated by adding (as shown in table). However, accuracy requires different means of calculation for longer duration flights. |
2. On the other hand, relativity will definitely affect interstellar flights. Even with g-force acceleration, those flights will take years. After 300 days of g-force acceleration, we will have not even approached the Oort Cloud, but we speculate that spaceship's velocity will be .866c. At this relativistic speed, spaceship's mass doubles, and inflight time shrinks by 50%. By the time, we'll doing interstellar missions, we'll likely have some solutions for this phenomena. |
|
SUMMARY: Equivalent Expressions of g Above expressions have nearly equal values; all approximate g, acceleration due to gravity at Earth surface. Recall that g is an acceleration which is velocity per time. Above expressions are all stated as velocity per unit time.
|
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