John Herschel Glenn, Jr.
First first American to orbit the Earth, and later, the oldest person to make a spaceflight.
( Born July 18, 1921) is a retired United States Marine Corps pilot, astronaut, and United States senator. He was a combat aviator in the Marine Corps, and now the only surviving member of the Mercury Seven; the elite U.S. military test pilots selected by NASA to operate the experimental Mercury spacecraft and become the first American astronauts.
On February 20, 1962, Glenn flew the Friendship 7 mission and became the first American to orbit the Earth and the fifth person in space, after cosmonauts Yuri Gagarin and Gherman Titov and the suborbital missions of fellow Mercury Seven astronauts Alan Shepard and Gus Grissom. In 1965, Glenn retired from the military and resigned from NASA so he could be eligible to stand for election to public office. As a member of the Democratic Party he was elected to represent Ohio in the U.S. Senate from 1974 to 1999.Glenn received a Congressional Space Medal of Honor in 1978, and the Presidential Medal of Freedom in 2012. He was inducted into the Astronaut Hall of Fame in 1990. On October 29, 1998, while still a sitting senator, he became the oldest person to fly in space, and the only one to fly in both the Mercury and Space Shuttle programs, when at age 77, he flew on Discovery (STS-95). With the death of Scott Carpenter on October 10, 2013, Glenn is the last surviving member of the Mercury Seven
Sigmund Werner Paul Jähn
First German in space ..
(Born 13 February 1937) is a German pilot, who became the first German to fly in space as part of the Soviet Union's Interkosmos programme.
Jähn was born in
Morgenröthe-Rautenkranz, in
the Vogtland
district of Saxony, Germany. From 1943
to 1951 he
attended school
in his hometown, and after school trained as a
printer.
In 1955 he joined
the East German Air
Force, where he became a pilot and military scientist.
From 1966 until 1970
he studied at the
Gagarin Air Force Academy
in Monino, in the Soviet Union, and
afterwards worked in the
administration of
the East German air force, responsible for pilot education
and
flight
safety.Jähn was awarded
the title Hero of the Soviet Union on
3
September 1978.In
1983 he received
a doctorate in
physics at the
Zentralinstitut für Physik
der Erde (de)
in Potsdam, specialising in
remote
sensing of the
earth.
In 1976, Jähn was selected with his backup Eberhard Köllner for the Interkosmos programme. He trained in Star City near Moscow for the next two years, and flew on board Soyuz 31 (launched 26 August 1978) to the Soviet space station Salyut 6, and returned on Soyuz 29, landing on 3 September 1978. He spent 7 days, 20 hours, and 49 minutes in space.During and after the flight, he and the socialist authorities of the GDR pronounced him "the first German cosmonaut", which was remarkable, as in those days .the East German state normally stressed that their people were "GDR citizens", to distinguish themselves from West Germany.
Chiaki Mukai
First Japanese Woman in space .
(Born on May 6, 1952, Tatebayashi, Gunma, Japan) is a Japanese doctor, and JAXA astronaut.She was the first Japanese woman in space, and was the first Japanese citizen to have two spaceflights.[Both were Space Shuttle missions; her first was STS-65 aboard Space Shuttle Columbia in July 1994, which was a Spacelab mission. Her second spaceflight was STS-95 aboard Space Shuttle Discovery in 1998. In total she has spent 23 days in space.
Mukai was selected to be an astronaut by Japanese national space agency NASDA (now called JAXA) in 1985. Prior to this, she was an assistant professor in the Department of Cardiovascular Surgery in Keio University, the oldest university in Japan.
In 1985, Mukai was selected as one of three Japanese Payload Specialist candidates for the First Material Processing Test (Spacelab-J) which flew aboard STS-47. She also served as a back-up payload specialist for the Neurolab (STS-90) mission. Mukai has logged over 566 hours in space. She flew aboard STS-65 in 1994 and STS-95 in 1998. She is the first Japanese woman to fly in space, and the first Japanese citizen to fly twice.As a NASDA astronaut, she was a visiting scientist at the Division of Cardiovascular Physiology, Space Biomedical Research Institute, NASA Johnson Space Center, from 1987 to 1988. Mukai has remained a Research Instructor of the Department of Surgery, Baylor College of Medicine, Houston, Texas, since 1992. From 1992 to 1998 she was a visiting associate professor of the Department of Surgery, Keio University School of Medicine, Tokyo, and in 1999 was promoted to a visiting professor of the university.Mukai was assigned the deputy mission scientist for STS-107. In that capacity she coordinated science operations for this science mission. In 2009 Mukai was a visiting lecturer at the International Space University
Rodolfo Neri Vela
First Maxican in space
(Born 19 February 1952) is a Mexican
scientist and astronaut who flew aboard a
NASA
Space Shuttle mission in
the year 1985.[1] He is the first
and only Mexican, and the second Latin-American to have traveled to
space.Neri received
a bachelor's degree in
mechanical and electrical engineering,
National Autonomous University of
Mexico (UNAM) 1975, and received a master's degree in science,
specialized in telecommunications systems,
in 1976 from the University of Essex,
England. Neri then received
a doctorate degree in
electromagnetic radiation
from the University of Birmingham in
1979, and performed one year of postdoctoral research in waveguides
at the University of
Birmingham.Neri
was a Payload Specialist aboard
the STS-61-B
Atlantis
mission,
from (November 26 to December 3, 1985).STS-61B
launched
at night from Kennedy Space Center,
Florida, and returned to
land at Edwards Air Force Base,
California.
During
the mission the crew deployed the MORELOS-B,
AUSSATT II, and
SATCOM K-2 communications satellites, conducted two
six-hour spacewalks to monstrate
space station
construction
techniques
with the EASE/ACCESS experiments, operated the Continuous
Flow
Electrophoresis
(CRFES) experiment for McDonell Douglas and
a
Getaway Special (GAS) container for
Telesat, Canada, conducted several
Mexican Payload Specialists
Experiments for the Mexican
government, and tested the Orbiter Experiments Digital Autopilot (OEX
DAP). At mission conclusion, Neri had
traveled 2.4 million miles (3.8 million km)
in 108
Earth orbits, and logged over 165 hours in
space
GRAVITY
Gravitation, or gravity, is a natural phenomenon by which all
physical bodies attract each other. It is most commonly recognized
and experienced as the agent that gives weight to physical objects
and causes physical objects to fall toward the ground when dropped
from a height.
Gravity of other planet :
1] Earth : 0.98 ( Moon-0.17 )
2] Mercury :0.38
3] Neptune : 1.13
4] Jupetor : 24.79
5] Mars : 3.711
6] Pluto : 0.658
7] Saturan : 0.92
8] Uranus : 0.89
9] Venus :0.90
Newton's Theory of Gravitation :
In 1687, English mathematician Sir Isaac Newton published
Principia, which hypothesizes the inverse-square law of universal
gravitation. In his own words, “I deduced that the forces which
keep the planets in their orbs must [be] reciprocally as the
squares of their distances from the centers about which they
revolve: and thereby compared the force requisite to keep the Moon
in her Orb with the force of gravity at the surface of the Earth;
and found them answer pretty nearly.”
Newton's theory enjoyed its greatest success when it was used to
predict the existence of Neptune based on motions of Uranus that
could not be accounted for by the actions of the other planets.
Calculations by both John Couch Adams and Urbain Le Verrier
predicted the general position of the planet, and Le Verrier's
calculations are what led Johann Gottfried Galle to the discovery
of Neptune.
A discrepancy in Mercury's orbit pointed out flaws in Newton's
theory. By the end of the 19th century, it was known that its orbit
showed slight perturbations that could not be accounted for
entirely under Newton's theory, but all searches for another
perturbing body (such as a planet orbiting the Sun even closer than
Mercury) had been fruitless. The issue was resolved in 1915 by
Albert Einstein's new theory of general relativity, which accounted
for the small discrepancy in Mercury's orbit.
Although Newton's theory has been superseded, most modern
non-relativistic gravitational calculations are still made using
Newton's theory because it is a much simpler theory to work with
than general relativity, and gives sufficiently accurate results
for most applications involving sufficiently small masses, speeds
and Gravitational force .
Gravitational Force:
Law of Universal
Gravitation:
Every particle attracts every other particle with a force that is
proportional to the mass of the particles and inversely
proportional to the square of the distance between them.
F directly propotional to mM/d2 .
The sign means “proportional to.” To make an equation out of the
above situation, insert a quantity called the universal constant of
gravitation,G.
G 6.67 1011 Nm2/kg2
Now the magnitude of this gravitational force can be represented as
Force = ( universal constant of gravitation)2 (1mass) (mass2 )/
(distance)2
F = GmM/d2
Like all other forces, the gravitational force of attraction
between two objects is measured in newtons.
Gravitational Acceleration :
Newton's laws of universal gravitation states that their is force F
of attraction between two particle of mass m1 and m2 separated by
adistance r that is represented by relationship
F = (( Gm1m2)/r2)
were G is universal gravitational constant . the value 'G' first
determine in 1798 by Lord Cavendish is 6.6732x10(-11) nt.m2/kg2 the
present value which is determine in 1942.
Gravitation Equation
:
Now suppose our boundary is not innitely extended, but forms a closed surface. More specically, let us assume it is a sphere. For the following it is best to forget about the Unruh law , since we don't need it. It only served as a further motivation for ). The key statement is simply that we need to have a temperature in order to have a force. Since we want to understand the origin of the force, we need to know where the temperature comes from. One can think about the boundary as a storage device for information. Assuming that the holographic principle holds, the maximal storage space, or total number of mbits, is proportional to the area A. In fact, in an theory of emergent space this how area may be dened: each fundamental bit occupies by denition one unit cell. Let us denote the number of used bits by N. It is natural to assume that this number will be proportional to the area.
So we write N =Ac3/Gh
where we introduced a new constant G. Eventually this constant is
going to be identied with Newton's constant, of course. But since
we have not assumed anything yet about the existence a
gravitational force, one can simply regard this equation as
the denition of G. So, the only assumption made here is that the
number of bits is proportional to the area. Nothing more. Suppose
there is a total energy E present in the system. Let us now just
make the simple assumption that the energy is divided evenly over
the bits N. The temperature
is then determined by the equipartition rule E =1/2 (NkBT
).
as the average energy per bit. After this we need only one more
equation:E = Mc2:
Here M represents the mass that would emerge in the part of space
enclosed by the screen, see gure 3. Even though the mass is not
directly visible in the emerged space, its presence is noticed
though its energy.The rest is straightforward: one eliminates E and
inserts the expression for the number of bits to determine
T.
Next one uses the postulate for the change of entropy to determine
the force.
Finally one inserts A = 4R2:
and one obtains the familiar law: F = GMm/R2 :
We have recovered Newton's law of gravitation, practically from rst
principles! These equations do not just come out by accident. It
had to work, partly for dimensional reasons, and also because the
laws of Newton have been ingredients in the steps that lead to
black hole thermodynamics and the holographic principle. In a sense
we have reversed these arguments. But the logic is clearly dierent,
and sheds new light on the origin of gravity: it is an entropic
force! That is the main statement, which is new and has not been
made before.
Gravitation Equation for body failing near earth surface :
Under an assumption of constant gravity, Newton's law of universal
gravitation simplifies to F = mg, where m is the mass of the body
and g is a constant vector with an average magnitude of 9.81 m/s2.
The acceleration due to gravity is equal to this g. An initially
stationary object which is allowed to fall freely under gravity
drops a distance which is proportional to the square of the elapsed
time. The image on the right, spanning half a second, was captured
with a stroboscopic flash at 20 flashes per second. During the
first 1/20 of a second the ball drops one unit of distance (here, a
unit is about 12 mm); by 2/20 it has dropped at total of 4 units;
by 3/20, 9 units and so on.
Under the same constant gravity assumptions, the potential energy,
Ep, of a body at height h is given by Ep = mgh (or Ep = Wh, with W
meaning weight). This expression is valid only over small distances
h from the surface of the Earth. Similarly, the expression h =
\tfrac{v^2}{2g} for the maximum height reached by a vertically
projected body with initial velocity v is useful for small heights
and small initial velocities only.
Earth Gravitation field :
Every planetary body (including the Earth) is surrounded by its own
gravitational field, which exerts an attractive force on all
objects. Assuming a spherically symmetrical planet, the strength of
this field at any given point is proportional to the planetary
body's mass and inversely proportional to the square of the
distance from the center of the body.
The strength of the gravitational field is numerically equal to the
acceleration of objects under its influence, and its value at the
Earth's surface, denoted g, is expressed below as the standard
average. According to the Bureau International de Poids et Mesures,
International Systems of Units (SI), the Earth's standard
acceleration due to gravity is:
g = 9.80665 m/s2 (32.1740 ft/s2).
This means that, ignoring air resistance, an object falling freely
near the Earth's surface increases its velocity by 9.80665 m/s
(32.1740 ft/s or 22 mph) for each second of its descent. Thus, an
object starting from rest will attain a velocity of 9.80665 m/s
(32.1740 ft/s) after one second, approximately 19.62 m/s (64.4
ft/s) after two seconds, and so on, adding 9.80665 m/s (32.1740
ft/s) to each resulting velocity. Also, again ignoring air
resistance, any and all objects, when dropped from the same height,
will hit the ground at the same time.