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Einstein tried and failed at this endeavor, but currently the most popular approach to answering this question is string theory.

What we now call gravity was not identified as a universal force until the work of Isaac Newton. Before Newton, the tendency for objects to fall towards the Earth was not understood to be related to the motions of celestial objects.

Galileo was instrumental in describing the characteristics of falling objects by determining that the acceleration of every object in free-fall was constant and independent of the mass of the object.

For an object in free-fall, this force is unopposed and the net force on the object is its weight. For objects not in free-fall, the force of gravity is opposed by the reaction forces applied by their supports.

For example, a person standing on the ground experiences zero net force, since a normal force a reaction force is exerted by the ground upward on the person that counterbalances his weight that is directed downward.

Newton's contribution to gravitational theory was to unify the motions of heavenly bodies, which Aristotle had assumed were in a natural state of constant motion, with falling motion observed on the Earth.

He proposed a law of gravity that could account for the celestial motions that had been described earlier using Kepler's laws of planetary motion.

Newton came to realize that the effects of gravity might be observed in different ways at larger distances. In particular, Newton determined that the acceleration of the Moon around the Earth could be ascribed to the same force of gravity if the acceleration due to gravity decreased as an inverse square law.

Further, Newton realized that the acceleration of a body due to gravity is proportional to the mass of the other attracting body. This constant has come to be known as Newton's Universal Gravitation Constant , [28] though its value was unknown in Newton's lifetime.

Newton, however, realized that since all celestial bodies followed the same laws of motion , his law of gravity had to be universal.

This formula was powerful enough to stand as the basis for all subsequent descriptions of motion within the solar system until the 20th century.

During that time, sophisticated methods of perturbation analysis [29] were invented to calculate the deviations of orbits due to the influence of multiple bodies on a planet , moon , comet , or asteroid.

The formalism was exact enough to allow mathematicians to predict the existence of the planet Neptune before it was observed.

Mercury 's orbit, however, did not match that predicted by Newton's Law of Gravitation. Some astrophysicists predicted the existence of another planet Vulcan that would explain the discrepancies; however no such planet could be found.

When Albert Einstein formulated his theory of general relativity GR he turned his attention to the problem of Mercury's orbit and found that his theory added a correction, which could account for the discrepancy.

This was the first time that Newton's Theory of Gravity had been shown to be inexact. Since then, general relativity has been acknowledged as the theory that best explains gravity.

In GR, gravitation is not viewed as a force, but rather, objects moving freely in gravitational fields travel under their own inertia in straight lines through curved space-time — defined as the shortest space-time path between two space-time events.

From the perspective of the object, all motion occurs as if there were no gravitation whatsoever. It is only when observing the motion in a global sense that the curvature of space-time can be observed and the force is inferred from the object's curved path.

Thus, the straight line path in space-time is seen as a curved line in space, and it is called the ballistic trajectory of the object. For example, a basketball thrown from the ground moves in a parabola , as it is in a uniform gravitational field.

Its space-time trajectory is almost a straight line, slightly curved with the radius of curvature of the order of few light-years. The time derivative of the changing momentum of the object is what we label as "gravitational force".

The electrostatic force was first described in by Coulomb as a force that existed intrinsically between two charges. Coulomb's law unifies all these observations into one succinct statement.

Subsequent mathematicians and physicists found the construct of the electric field to be useful for determining the electrostatic force on an electric charge at any point in space.

The electric field was based on using a hypothetical " test charge " anywhere in space and then using Coulomb's Law to determine the electrostatic force.

Meanwhile, the Lorentz force of magnetism was discovered to exist between two electric currents. It has the same mathematical character as Coulomb's Law with the proviso that like currents attract and unlike currents repel.

Similar to the electric field, the magnetic field can be used to determine the magnetic force on an electric current at any point in space.

In this case, the magnitude of the magnetic field was determined to be. The magnetic field exerts a force on all magnets including, for example, those used in compasses.

The fact that the Earth's magnetic field is aligned closely with the orientation of the Earth's axis causes compass magnets to become oriented because of the magnetic force pulling on the needle.

Through combining the definition of electric current as the time rate of change of electric charge, a rule of vector multiplication called Lorentz's Law describes the force on a charge moving in a magnetic field.

This force can be written as a sum of the electrostatic force due to the electric field and the magnetic force due to the magnetic field.

Fully stated, this is the law:. The origin of electric and magnetic fields would not be fully explained until when James Clerk Maxwell unified a number of earlier theories into a set of 20 scalar equations, which were later reformulated into 4 vector equations by Oliver Heaviside and Josiah Willard Gibbs.

This led Maxwell to discover that electric and magnetic fields could be "self-generating" through a wave that traveled at a speed that he calculated to be the speed of light.

This insight united the nascent fields of electromagnetic theory with optics and led directly to a complete description of the electromagnetic spectrum.

However, attempting to reconcile electromagnetic theory with two observations, the photoelectric effect , and the nonexistence of the ultraviolet catastrophe , proved troublesome.

Through the work of leading theoretical physicists, a new theory of electromagnetism was developed using quantum mechanics.

This final modification to electromagnetic theory ultimately led to quantum electrodynamics or QED , which fully describes all electromagnetic phenomena as being mediated by wave—particles known as photons.

In QED, photons are the fundamental exchange particle, which described all interactions relating to electromagnetism including the electromagnetic force.

There are two " nuclear forces ", which today are usually described as interactions that take place in quantum theories of particle physics.

The strong nuclear force [16] : is the force responsible for the structural integrity of atomic nuclei while the weak nuclear force [16] : is responsible for the decay of certain nucleons into leptons and other types of hadrons.

The strong force is today understood to represent the interactions between quarks and gluons as detailed by the theory of quantum chromodynamics QCD.

The aptly named strong interaction is the "strongest" of the four fundamental forces. The strong force only acts directly upon elementary particles.

However, a residual of the force is observed between hadrons the best known example being the force that acts between nucleons in atomic nuclei as the nuclear force.

Here the strong force acts indirectly, transmitted as gluons, which form part of the virtual pi and rho mesons , which classically transmit the nuclear force see this topic for more.

The failure of many searches for free quarks has shown that the elementary particles affected are not directly observable.

This phenomenon is called color confinement. The weak force is due to the exchange of the heavy W and Z bosons. Its most familiar effect is beta decay of neutrons in atomic nuclei and the associated radioactivity.

The word "weak" derives from the fact that the field strength is some 10 13 times less than that of the strong force.

Still, it is stronger than gravity over short distances. Such temperatures have been probed in modern particle accelerators and show the conditions of the universe in the early moments of the Big Bang.

Some forces are consequences of the fundamental ones. In such situations, idealized models can be utilized to gain physical insight. The normal force is due to repulsive forces of interaction between atoms at close contact.

When their electron clouds overlap, Pauli repulsion due to fermionic nature of electrons follows resulting in the force that acts in a direction normal to the surface interface between two objects.

An example of the normal force in action is the impact force on an object crashing into an immobile surface. Friction is a surface force that opposes relative motion.

The frictional force is directly related to the normal force that acts to keep two solid objects separated at the point of contact. There are two broad classifications of frictional forces: static friction and kinetic friction.

In other words, the magnitude of the static friction force satisfies the inequality:. Thus, the magnitude of the force equals:.

For most surface interfaces, the coefficient of kinetic friction is less than the coefficient of static friction. Tension forces can be modeled using ideal strings that are massless, frictionless, unbreakable, and unstretchable.

They can be combined with ideal pulleys , which allow ideal strings to switch physical direction. Ideal strings transmit tension forces instantaneously in action-reaction pairs so that if two objects are connected by an ideal string, any force directed along the string by the first object is accompanied by a force directed along the string in the opposite direction by the second object.

For every string that acts on a load, another factor of the tension force in the string acts on the load. However, even though such machines allow for an increase in force , there is a corresponding increase in the length of string that must be displaced in order to move the load.

These tandem effects result ultimately in the conservation of mechanical energy since the work done on the load is the same no matter how complicated the machine.

An elastic force acts to return a spring to its natural length. An ideal spring is taken to be massless, frictionless, unbreakable, and infinitely stretchable.

Such springs exert forces that push when contracted, or pull when extended, in proportion to the displacement of the spring from its equilibrium position.

The minus sign accounts for the tendency of the force to act in opposition to the applied load. Newton's laws and Newtonian mechanics in general were first developed to describe how forces affect idealized point particles rather than three-dimensional objects.

However, in real life, matter has extended structure and forces that act on one part of an object might affect other parts of an object.

For situations where lattice holding together the atoms in an object is able to flow, contract, expand, or otherwise change shape, the theories of continuum mechanics describe the way forces affect the material.

For example, in extended fluids , differences in pressure result in forces being directed along the pressure gradients as follows:.

Pressure gradients and differentials result in the buoyant force for fluids suspended in gravitational fields, winds in atmospheric science , and the lift associated with aerodynamics and flight.

A specific instance of such a force that is associated with dynamic pressure is fluid resistance: a body force that resists the motion of an object through a fluid due to viscosity.

For so-called " Stokes' drag " the force is approximately proportional to the velocity, but opposite in direction:.

More formally, forces in continuum mechanics are fully described by a stress — tensor with terms that are roughly defined as.

This formalism includes pressure terms associated with forces that act normal to the cross-sectional area the matrix diagonals of the tensor as well as shear terms associated with forces that act parallel to the cross-sectional area the off-diagonal elements.

The stress tensor accounts for forces that cause all strains deformations including also tensile stresses and compressions.

There are forces that are frame dependent , meaning that they appear due to the adoption of non-Newtonian that is, non-inertial reference frames.

Such forces include the centrifugal force and the Coriolis force. In general relativity , gravity becomes a fictitious force that arises in situations where spacetime deviates from a flat geometry.

As an extension, Kaluza—Klein theory and string theory ascribe electromagnetism and the other fundamental forces respectively to the curvature of differently scaled dimensions, which would ultimately imply that all forces are fictitious.

Forces that cause extended objects to rotate are associated with torques. Torque is the rotation equivalent of force in the same way that angle is the rotational equivalent for position , angular velocity for velocity , and angular momentum for momentum.

As a consequence of Newton's First Law of Motion, there exists rotational inertia that ensures that all bodies maintain their angular momentum unless acted upon by an unbalanced torque.

Likewise, Newton's Second Law of Motion can be used to derive an analogous equation for the instantaneous angular acceleration of the rigid body:.

This provides a definition for the moment of inertia, which is the rotational equivalent for mass. In more advanced treatments of mechanics, where the rotation over a time interval is described, the moment of inertia must be substituted by the tensor that, when properly analyzed, fully determines the characteristics of rotations including precession and nutation.

Equivalently, the differential form of Newton's Second Law provides an alternative definition of torque:. Newton's Third Law of Motion requires that all objects exerting torques themselves experience equal and opposite torques, [43] and therefore also directly implies the conservation of angular momentum for closed systems that experience rotations and revolutions through the action of internal torques.

For an object accelerating in circular motion, the unbalanced force acting on the object equals: [44]. This means that the unbalanced centripetal force felt by any object is always directed toward the center of the curving path.

Such forces act perpendicular to the velocity vector associated with the motion of an object, and therefore do not change the speed of the object magnitude of the velocity , but only the direction of the velocity vector.

The unbalanced force that accelerates an object can be resolved into a component that is perpendicular to the path, and one that is tangential to the path.

This yields both the tangential force, which accelerates the object by either slowing it down or speeding it up, and the radial centripetal force, which changes its direction.

Forces can be used to define a number of physical concepts by integrating with respect to kinematic variables. For example, integrating with respect to time gives the definition of impulse : [45].

Similarly, integrating with respect to position gives a definition for the work done by a force: [3] : 13—3. Instead of a force, often the mathematically related concept of a potential energy field can be used for convenience.

For instance, the gravitational force acting upon an object can be seen as the action of the gravitational field that is present at the object's location.

Forces can be classified as conservative or nonconservative. Conservative forces are equivalent to the gradient of a potential while nonconservative forces are not.

A conservative force that acts on a closed system has an associated mechanical work that allows energy to convert only between kinetic or potential forms.

This means that for a closed system, the net mechanical energy is conserved whenever a conservative force acts on the system. The force, therefore, is related directly to the difference in potential energy between two different locations in space, [46] and can be considered to be an artifact of the potential field in the same way that the direction and amount of a flow of water can be considered to be an artifact of the contour map of the elevation of an area.

Conservative forces include gravity , the electromagnetic force, and the spring force. For certain physical scenarios, it is impossible to model forces as being due to gradient of potentials.

This is often due to macrophysical considerations that yield forces as arising from a macroscopic statistical average of microstates.

For example, friction is caused by the gradients of numerous electrostatic potentials between the atoms , but manifests as a force model that is independent of any macroscale position vector.

Nonconservative forces other than friction include other contact forces , tension , compression , and drag. However, for any sufficiently detailed description, all these forces are the results of conservative ones since each of these macroscopic forces are the net results of the gradients of microscopic potentials.

The connection between macroscopic nonconservative forces and microscopic conservative forces is described by detailed treatment with statistical mechanics.

In macroscopic closed systems, nonconservative forces act to change the internal energies of the system, and are often associated with the transfer of heat.

According to the Second law of thermodynamics , nonconservative forces necessarily result in energy transformations within closed systems from ordered to more random conditions as entropy increases.

The gravitational foot-pound-second English unit of force is the pound-force lbf , defined as the force exerted by gravity on a pound-mass in the standard gravitational field of 9.

An alternative unit of force in a different foot-pound-second system, the absolute fps system, is the poundal , defined as the force required to accelerate a one-pound mass at a rate of one foot per second squared.

The pound-force has a metric counterpart, less commonly used than the newton: the kilogram-force kgf sometimes kilopond , is the force exerted by standard gravity on one kilogram of mass.

The kilogram-force is not a part of the modern SI system, and is generally deprecated; however it still sees use for some purposes as expressing aircraft weight, jet thrust, bicycle spoke tension, torque wrench settings and engine output torque.

See force gauge , spring scale , load cell. From Wikipedia, the free encyclopedia. For other uses, see Force disambiguation. Any action that tends to maintain or alter the motion of an object.

Forces can be described as a push or pull on an object. They can be due to phenomena such as gravity , magnetism , or anything that might cause a mass to accelerate.

Second law of motion. History Timeline Textbooks. Newton's laws of motion. Analytical mechanics Lagrangian mechanics Hamiltonian mechanics Routhian mechanics Hamilton—Jacobi equation Appell's equation of motion Koopman—von Neumann mechanics.

Core topics. Circular motion Rotating reference frame Centripetal force Centrifugal force reactive Coriolis force Pendulum Tangential speed Rotational speed.

See also: Aristotelian physics and Theory of impetus. Main article: Newton's laws of motion. Main article: Newton's first law.

Main article: Newton's second law. Main article: Newton's third law. Main articles: Statics and Static equilibrium. Main article: Dynamics physics.

Main articles: Quantum mechanics and Pauli exclusion principle. Main article: Feynman diagrams. Main article: Fundamental interaction. Main article: Gravity.

Main article: Electromagnetic force. Main article: Strong interaction. Main article: Weak interaction. Main article: Normal force.

Main article: Friction. Main article: Tension physics. Main articles: Elasticity physics and Hooke's law. Main articles: Pressure , Drag physics , and Stress mechanics.

Main article: Fictitious forces. Main article: Torque. Main article: Centripetal force. Main articles: Impulse , Mechanical work , and Power physics.

Main article: Potential energy. Main article: Conservative force. Physics portal. See Impulse. The Works of Archimedes Internet Archive.

Retrieved Dreams of a Final Theory. Vintage Books. Cambridge: Cambridge Univ. Garland Reference Library of the Humanities.

Galileo At Work. Chicago: University of Chicago Press. Berkeley: University of California Press. This is a recent translation into English by I.

Intermediate dynamics a linear algebraic approach Online-Ausg. New York: Springer. General Physics; mechanics and molecular physics First English ed.

Oxford: Pergamon Press. Translated by: J. Sykes, A. Petford, and C. In section 7, pp. Mineola, N. Carnegie Mellon University.

Retrieved 28 October Hellingman Bibcode : PhyEd.. Quoting Newton in the Principia : It is not one action by which the Sun attracts Jupiter, and another by which Jupiter attracts the Sun; but it is one action by which the Sun and Jupiter mutually endeavour to come nearer together.

Nikitin The Relativistic Raytracer. Archived from the original on 26 June Physics Tutorial Menu. University of Guelph. Archived from the original on Physics Static Equilibrium forces and torques.

University of the Virgin Islands. Archived from the original on October 19, ITEP lectures on particle physics and field theory.

World Scientific. The Particle Adventure. Contemporary Physics Education Project. Retrieved 2 January Bibcode : Natur. Pearson Education. Astronomy The Solar System.

Department of Economics. The British Case for Co-Prediction". University College London. Retrieved 13 August Retrieved 3 January Polarized light in liquid crystals and polymers.

John Wiley and Sons. Electricity and Magnetism, 3rd Ed. Non-Calculus Based Physics I. Publications in Science and Mathematics, Computing and the Humanities.

Inwit Publishing, Inc. Engineering Mechanics, 12th edition. Pearson Prentice Hall. General physics.

Metric Units in Engineering. ASCE Publications. Corben, H. Classical Mechanics. New York: Dover publications. Cutnell, John D.

Physics, Sixth Edition. The Feynman lectures on physics. I: Mainly mechanics, radiation and heat New millennium ed.

New York: BasicBooks. Feynman, Richard P. II: Mainly electromagnetism and matter New millennium ed. Physics v. An introduction to mechanics 3.

Cambridge: Cambridge University Press. Encyclopedia of Physics. Ohio: McGraw-Hill. Sears F. University Physics.

Reading, Massachusetts: Addison-Wesley. Serway, Raymond A. Physics for Scientists and Engineers. Philadelphia: Saunders College Publishing.

Tipler, Paul Verma, H. Concepts of Physics Vol 1 Reprint ed. Bharti Bhavan. The fundamental interactions of physics. Electromagnetic radiation Gravitational radiation.

Fifth force Quintessence Weak gravity conjecture. Classical mechanics SI units. Underwater diving. Diving equipment. Cleaning and disinfection of personal diving equipment Human factors in diving equipment design.

Are you familiar with the dark side of the Force or are you a Jedi Master? Movies a new hope , jedi , star wars. Have you ever bulls-eyed a womp rat?

May the Force be with you! Ever wish you could be a Jedi Master or a Sith Lord, battling it out with lightsabers? Of course you have! Take the quiz and find out if the Force is with you!

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By continuing to browse this site you are agreeing to our use of cookies. Is The Force With You? I want a cupcake No, thanks I'm not hungry What are you talking about?

Get it Try my hardest Ask for it for my birthday. It's in the movies It's up in the sky It's within all of us How should I know? What, are you crazy?

I have actually I know I'm going to go to the next question. What are they? Give up and just watch whatever infomercial is on Get up and grab it Try to move it with my mind

Scientific American. Newton's laws of motion. The A. In Aristotle's view, the terrestrial sphere contained four elements that come to rest at different "natural places" therein. Science of underwater diving. Scarecrow Press. In section 7, pp. Retrieved December 24, Life : Summing these component forces using vector Beste Spielothek in Ludmerfeld finden yields the original force. The Force Is With You

The Force Is With You Inhaltsverzeichnis

May the force be with you! Griechisch Wörterbücher. Der Film läuft auch in 3D, was den visuellen Reiz noch erhöht. Palpatine soll eine neue Kampfflotte parat halten, die mit ihrer unglaublichen Feuerkraft alle rebellische Völker im Universum vernichten kann, samt ihrer Planeten. In diesem Sinne : Möge die Macht mit deinem Bart sein! This Beste Spielothek in Pfaffenrot finden where the work of the church film organisations and yours are essentially linked. Möchten Sie ein Wort, eine Phrase Paysafecard Mindestalter eine Übersetzung hinzufügen? JJ Abrams führt Regie, genau wie zuvor in Episode 7. Ergebnisse: May the crochet-hook be with you!. Februar Published by Robert Eiba at May our values be with you. Ne plus afficher ce message. Fans selbst Regierungsvertreter 1100 Spiele haben Star Wars auf eine vielfältige Weise in den sozialen Medien und im Fernsehen gefeiert. Registrieren Einloggen. Der Eintrag wurde Ihren Favoriten hinzugefügt. August Einzig ein altes Navigationsgerät der Sith könnte die Rebellen dorthin führen. Nein, möge die Macht mit dir seinJ. Es ist ein Fehler aufgetreten. Möge die Macht mir Dir sein. JJ Abrams führt Regie, genau wie zuvor in Episode 7. More than Scatter Slot feeling Übersetzung Lyrics : Ich will bei dir sein Einfach nur bei dir sein Wie kann ich bei dir sein, Baby?

And then there is that distressing thing called the Force, which is Lucas's tribute to something beyond science: imagination, the soul, God in man It appears in various contradictory and finally nonsensical guises, a facile and perfunctory bow to metaphysics.

I wish that Lucas had had the courage of his materialistic convictions, instead dragging in a sop to a spiritual force the main thrust of the movie so cheerfully ignores.

Critic Tim Robley compared the Force to the ruby slippers from The Wizard of Oz , with both being entities that send the protagonist on a quest.

It doesn't seem to be connected with ethics or a code of decent behavior, either. The introduction of midi-chlorians in The Phantom Menace was controversial, with Evan Narcisse of Time writing that the concept ruined Star Wars for him and a generation of fans because "the mechanisms of the Force became less spiritual and more scientific".

Caputo writes, "In the 'Gospel according to Lucas' a world is conjured up in which the intractable oppositions that have tormented religious thinkers for centuries are reconciled The gifts that the Jedi masters enjoy have a perfectly plausible scientific basis, even if its ways are mysterious".

Characters' faith in the Force reinforces the Rogue One ' s message of hope. Several Star Wars characters say " May the Force be with you " or derivatives of it and the expression has become a popular catchphrase.

President Ronald Reagan in said "the Force is with us", referring to the United States , to create the Strategic Defense Initiative to protect against Soviet ballistic missiles.

Moreover, the [ Star Wars ] blessing is precisely a request for hope for others " May the Force be with you" , whereas Reagan's claim sounds like a possessive assertion "The Force is with us".

From Wikipedia, the free encyclopedia. Redirected from May the Force be with you. This article is about the Mysterious power in the Star Wars universe.

For other uses, see The Force disambiguation. Fictional energy source in Star Wars. That energy surrounds us; when we die, that energy joins with all the other energy.

There is a giant mass of energy in the universe that has a good side and a bad side. We are part of the Force because we generate the power that makes the Force live.

When we die, we become part of that Force, so we never really die; we continue as part of the Force. See also: Cultural impact of Star Wars.

For other uses, see May the Force be with you disambiguation. Speculative fiction portal Film portal. Random House. Retrieved May 23, June 24, Star Wars.

Retrieved May 16, Retrieved May 25, Retrieved March 17, Retrieved May 15, The Guardian. Abrams explains why anyone would still want to join the new Empire in 'Star Wars ' ".

The Los Angeles Times. Los Angeles Times. Ross Levinsohn. Retrieved December 27, Retrieved September 16, Retrieved September 25, Retrieved February 25, Archived from the original on September 15, Retrieved August 31, New York: Ballantine Books.

The Huffington Post. Archived from the original on April 8, June 2, Event occurs at 10m, 40s. Retrieved May 26, Retrieved July 19, Retrieved May 24, Time Inc.

Peter Sciretta. Retrieved January 3, Star Wars: The Magic of Myth. Bantam Books. The Hollywood Reporter. Retrieved January 5, The Heritage Foundation.

Entertainment Weekly. Retrieved December 24, The Telegraph. Retrieved December 29, The Daily Beast. Retrieved December 30, Click on image 5 of 18 with thumbnail of Ezra Bridger.

The New Yorker. The failure of many searches for free quarks has shown that the elementary particles affected are not directly observable.

This phenomenon is called color confinement. The weak force is due to the exchange of the heavy W and Z bosons. Its most familiar effect is beta decay of neutrons in atomic nuclei and the associated radioactivity.

The word "weak" derives from the fact that the field strength is some 10 13 times less than that of the strong force. Still, it is stronger than gravity over short distances.

Such temperatures have been probed in modern particle accelerators and show the conditions of the universe in the early moments of the Big Bang.

Some forces are consequences of the fundamental ones. In such situations, idealized models can be utilized to gain physical insight.

The normal force is due to repulsive forces of interaction between atoms at close contact. When their electron clouds overlap, Pauli repulsion due to fermionic nature of electrons follows resulting in the force that acts in a direction normal to the surface interface between two objects.

An example of the normal force in action is the impact force on an object crashing into an immobile surface.

Friction is a surface force that opposes relative motion. The frictional force is directly related to the normal force that acts to keep two solid objects separated at the point of contact.

There are two broad classifications of frictional forces: static friction and kinetic friction. In other words, the magnitude of the static friction force satisfies the inequality:.

Thus, the magnitude of the force equals:. For most surface interfaces, the coefficient of kinetic friction is less than the coefficient of static friction.

Tension forces can be modeled using ideal strings that are massless, frictionless, unbreakable, and unstretchable. They can be combined with ideal pulleys , which allow ideal strings to switch physical direction.

Ideal strings transmit tension forces instantaneously in action-reaction pairs so that if two objects are connected by an ideal string, any force directed along the string by the first object is accompanied by a force directed along the string in the opposite direction by the second object.

For every string that acts on a load, another factor of the tension force in the string acts on the load. However, even though such machines allow for an increase in force , there is a corresponding increase in the length of string that must be displaced in order to move the load.

These tandem effects result ultimately in the conservation of mechanical energy since the work done on the load is the same no matter how complicated the machine.

An elastic force acts to return a spring to its natural length. An ideal spring is taken to be massless, frictionless, unbreakable, and infinitely stretchable.

Such springs exert forces that push when contracted, or pull when extended, in proportion to the displacement of the spring from its equilibrium position.

The minus sign accounts for the tendency of the force to act in opposition to the applied load. Newton's laws and Newtonian mechanics in general were first developed to describe how forces affect idealized point particles rather than three-dimensional objects.

However, in real life, matter has extended structure and forces that act on one part of an object might affect other parts of an object.

For situations where lattice holding together the atoms in an object is able to flow, contract, expand, or otherwise change shape, the theories of continuum mechanics describe the way forces affect the material.

For example, in extended fluids , differences in pressure result in forces being directed along the pressure gradients as follows:. Pressure gradients and differentials result in the buoyant force for fluids suspended in gravitational fields, winds in atmospheric science , and the lift associated with aerodynamics and flight.

A specific instance of such a force that is associated with dynamic pressure is fluid resistance: a body force that resists the motion of an object through a fluid due to viscosity.

For so-called " Stokes' drag " the force is approximately proportional to the velocity, but opposite in direction:. More formally, forces in continuum mechanics are fully described by a stress — tensor with terms that are roughly defined as.

This formalism includes pressure terms associated with forces that act normal to the cross-sectional area the matrix diagonals of the tensor as well as shear terms associated with forces that act parallel to the cross-sectional area the off-diagonal elements.

The stress tensor accounts for forces that cause all strains deformations including also tensile stresses and compressions. There are forces that are frame dependent , meaning that they appear due to the adoption of non-Newtonian that is, non-inertial reference frames.

Such forces include the centrifugal force and the Coriolis force. In general relativity , gravity becomes a fictitious force that arises in situations where spacetime deviates from a flat geometry.

As an extension, Kaluza—Klein theory and string theory ascribe electromagnetism and the other fundamental forces respectively to the curvature of differently scaled dimensions, which would ultimately imply that all forces are fictitious.

Forces that cause extended objects to rotate are associated with torques. Torque is the rotation equivalent of force in the same way that angle is the rotational equivalent for position , angular velocity for velocity , and angular momentum for momentum.

As a consequence of Newton's First Law of Motion, there exists rotational inertia that ensures that all bodies maintain their angular momentum unless acted upon by an unbalanced torque.

Likewise, Newton's Second Law of Motion can be used to derive an analogous equation for the instantaneous angular acceleration of the rigid body:.

This provides a definition for the moment of inertia, which is the rotational equivalent for mass.

In more advanced treatments of mechanics, where the rotation over a time interval is described, the moment of inertia must be substituted by the tensor that, when properly analyzed, fully determines the characteristics of rotations including precession and nutation.

Equivalently, the differential form of Newton's Second Law provides an alternative definition of torque:.

Newton's Third Law of Motion requires that all objects exerting torques themselves experience equal and opposite torques, [43] and therefore also directly implies the conservation of angular momentum for closed systems that experience rotations and revolutions through the action of internal torques.

For an object accelerating in circular motion, the unbalanced force acting on the object equals: [44]. This means that the unbalanced centripetal force felt by any object is always directed toward the center of the curving path.

Such forces act perpendicular to the velocity vector associated with the motion of an object, and therefore do not change the speed of the object magnitude of the velocity , but only the direction of the velocity vector.

The unbalanced force that accelerates an object can be resolved into a component that is perpendicular to the path, and one that is tangential to the path.

This yields both the tangential force, which accelerates the object by either slowing it down or speeding it up, and the radial centripetal force, which changes its direction.

Forces can be used to define a number of physical concepts by integrating with respect to kinematic variables. For example, integrating with respect to time gives the definition of impulse : [45].

Similarly, integrating with respect to position gives a definition for the work done by a force: [3] : 13—3.

Instead of a force, often the mathematically related concept of a potential energy field can be used for convenience. For instance, the gravitational force acting upon an object can be seen as the action of the gravitational field that is present at the object's location.

Forces can be classified as conservative or nonconservative. Conservative forces are equivalent to the gradient of a potential while nonconservative forces are not.

A conservative force that acts on a closed system has an associated mechanical work that allows energy to convert only between kinetic or potential forms.

This means that for a closed system, the net mechanical energy is conserved whenever a conservative force acts on the system.

The force, therefore, is related directly to the difference in potential energy between two different locations in space, [46] and can be considered to be an artifact of the potential field in the same way that the direction and amount of a flow of water can be considered to be an artifact of the contour map of the elevation of an area.

Conservative forces include gravity , the electromagnetic force, and the spring force. For certain physical scenarios, it is impossible to model forces as being due to gradient of potentials.

This is often due to macrophysical considerations that yield forces as arising from a macroscopic statistical average of microstates.

For example, friction is caused by the gradients of numerous electrostatic potentials between the atoms , but manifests as a force model that is independent of any macroscale position vector.

Nonconservative forces other than friction include other contact forces , tension , compression , and drag. However, for any sufficiently detailed description, all these forces are the results of conservative ones since each of these macroscopic forces are the net results of the gradients of microscopic potentials.

The connection between macroscopic nonconservative forces and microscopic conservative forces is described by detailed treatment with statistical mechanics.

In macroscopic closed systems, nonconservative forces act to change the internal energies of the system, and are often associated with the transfer of heat.

According to the Second law of thermodynamics , nonconservative forces necessarily result in energy transformations within closed systems from ordered to more random conditions as entropy increases.

The gravitational foot-pound-second English unit of force is the pound-force lbf , defined as the force exerted by gravity on a pound-mass in the standard gravitational field of 9.

An alternative unit of force in a different foot-pound-second system, the absolute fps system, is the poundal , defined as the force required to accelerate a one-pound mass at a rate of one foot per second squared.

The pound-force has a metric counterpart, less commonly used than the newton: the kilogram-force kgf sometimes kilopond , is the force exerted by standard gravity on one kilogram of mass.

The kilogram-force is not a part of the modern SI system, and is generally deprecated; however it still sees use for some purposes as expressing aircraft weight, jet thrust, bicycle spoke tension, torque wrench settings and engine output torque.

See force gauge , spring scale , load cell. From Wikipedia, the free encyclopedia. For other uses, see Force disambiguation. Any action that tends to maintain or alter the motion of an object.

Forces can be described as a push or pull on an object. They can be due to phenomena such as gravity , magnetism , or anything that might cause a mass to accelerate.

Second law of motion. History Timeline Textbooks. Newton's laws of motion. Analytical mechanics Lagrangian mechanics Hamiltonian mechanics Routhian mechanics Hamilton—Jacobi equation Appell's equation of motion Koopman—von Neumann mechanics.

Core topics. Circular motion Rotating reference frame Centripetal force Centrifugal force reactive Coriolis force Pendulum Tangential speed Rotational speed.

See also: Aristotelian physics and Theory of impetus. Main article: Newton's laws of motion. Main article: Newton's first law.

Main article: Newton's second law. Main article: Newton's third law. Main articles: Statics and Static equilibrium.

Main article: Dynamics physics. Main articles: Quantum mechanics and Pauli exclusion principle.

Main article: Feynman diagrams. Main article: Fundamental interaction. Main article: Gravity. Main article: Electromagnetic force.

Main article: Strong interaction. Main article: Weak interaction. Main article: Normal force. Main article: Friction.

Main article: Tension physics. Main articles: Elasticity physics and Hooke's law. Main articles: Pressure , Drag physics , and Stress mechanics.

Main article: Fictitious forces. Main article: Torque. Main article: Centripetal force. Main articles: Impulse , Mechanical work , and Power physics.

Main article: Potential energy. Main article: Conservative force. Physics portal. See Impulse. The Works of Archimedes Internet Archive. Retrieved Dreams of a Final Theory.

Vintage Books. Cambridge: Cambridge Univ. Garland Reference Library of the Humanities. Galileo At Work. Chicago: University of Chicago Press.

Berkeley: University of California Press. This is a recent translation into English by I. Intermediate dynamics a linear algebraic approach Online-Ausg.

New York: Springer. General Physics; mechanics and molecular physics First English ed. Oxford: Pergamon Press. Translated by: J.

Sykes, A. Petford, and C. In section 7, pp. Mineola, N. Carnegie Mellon University. Retrieved 28 October Hellingman Bibcode : PhyEd..

Quoting Newton in the Principia : It is not one action by which the Sun attracts Jupiter, and another by which Jupiter attracts the Sun; but it is one action by which the Sun and Jupiter mutually endeavour to come nearer together.

Nikitin The Relativistic Raytracer. Archived from the original on 26 June Physics Tutorial Menu. University of Guelph.

Archived from the original on Physics Static Equilibrium forces and torques. University of the Virgin Islands. Archived from the original on October 19, ITEP lectures on particle physics and field theory.

World Scientific. The Particle Adventure. Contemporary Physics Education Project. Retrieved 2 January Bibcode : Natur.

Pearson Education. Astronomy The Solar System. Department of Economics. The British Case for Co-Prediction". University College London.

Retrieved 13 August Retrieved 3 January Polarized light in liquid crystals and polymers. John Wiley and Sons. Electricity and Magnetism, 3rd Ed.

Non-Calculus Based Physics I. Publications in Science and Mathematics, Computing and the Humanities. Inwit Publishing, Inc. Engineering Mechanics, 12th edition.

Pearson Prentice Hall. General physics. Metric Units in Engineering. ASCE Publications. Please enter a valid email address.

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