# Newton's laws of motion

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**Newton's laws of motion** are three basic laws of classical mechanics that describe the relationship between the motion of an object and the forces acting on it. These laws can be paraphrased as follows:

- A body remains at rest, or in motion at a constant speed in a straight line, unless acted upon by a force.
- When a body is acted upon by a force, the time rate of change of its momentum equals the force.
- If two bodies exert forces on each other, these forces have the same magnitude but opposite directions.
^{[2]}

The three laws of motion were first stated by Isaac Newton in his *Philosophiæ Naturalis Principia Mathematica* (*Mathematical Principles of Natural Philosophy*), originally published in 1687.^{[3]} Newton used them to investigate and explain the motion of many physical objects and systems, which laid the foundation for classical mechanics. In the time since Newton, the conceptual content of classical physics has been reformulated in alternative ways, involving different mathematical approaches that have yielded insights which were obscured in the original, Newtonian formulation. Limitations to Newton's laws have also been discovered; new theories are necessary when objects move at very high speeds (special relativity), are very massive (general relativity), or are very small (quantum mechanics).

## Prerequisites

Newton's laws are often stated in terms of *point* or *particle* masses, that is, bodies whose volume is negligible. This is a reasonable approximation for real bodies when the motion of internal parts can be neglected, and when the separation between bodies is much larger than the size of each. For instance, the Earth and the Sun can both be approximated as pointlike when considering the orbit of the former around the latter, but the Earth is not pointlike when considering activities on its surface.^{[note 1]}

The mathematical description of motion, or kinematics, is based on the idea of specifying positions using numerical coordinates. Movement is represented by these numbers changing over time: a body's trajectory is represented by a function that assigns to each value of a time variable the values of all the position coordinates. The simplest case is one-dimensional, that is, when a body is constrained to move only along a straight line. Its position can then be given by a single number, indicating where it is relative to some chosen reference point. For example, a body might be free to slide along a track that runs left to right, and so its location can be specified by its distance from a convenient zero point, or origin, with negative numbers indicating positions to the left and positive numbers indicating positions to the right. If the body's location as a function of time is , then its average velocity over the time interval from to is^{[6]}

*instantaneous*velocity, a measure of a body's speed and direction of movement at a single moment of time, rather than over an interval. One notation for the instantaneous velocity is to replace with the symbol , for example,

^{[7]}More carefully, the velocity and all other derivatives can be defined using the concept of a limit.

^{[6]}A function has a limit of at a given input value if the difference between and can be made arbitrarily small by choosing an input sufficiently close to . One writes,

*Acceleration*is to velocity as velocity is to position: it is the derivative of the velocity with respect to time.

^{[note 2]}Acceleration can likewise be defined as a limit:

*second derivative*of position,

^{[7]}often written .

Position, when thought of as a displacement from an origin point, is a vector: a quantity with both magnitude and direction.^{[9]}^{: 1 } Velocity and acceleration are vector quantities as well. The mathematical tools of vector algebra provide the means to describe motion in two, three or more dimensions. Vectors are often denoted with an arrow, as in , or in bold typeface, such as . Often, vectors are represented visually as arrows, with the direction of the vector being the direction of the arrow, and the magnitude of the vector indicated by the length of the arrow. Numerically, a vector can be represented as a list; for example, a body's velocity vector might be , indicating that it is moving at 3 metres per second along a horizontal axis and 4 metres per second along the vertical axis. The same motion described in a different coordinate system will be represented by different numbers, and vector algebra can be used to translate between these alternatives.^{[9]}^{: 4 }

The physics concept of *force* makes quantitative the everyday idea of a push or a pull.^{[note 3]} Forces in Newtonian mechanics are often due to strings and ropes, friction, muscle effort, gravity, and so forth. Like displacement, velocity, and acceleration, force is a vector quantity.

## Laws

### First

Translated from the Latin, Newton's first law reads,

*Every body continues in its state of rest, or of uniform motion in a straight line, unless it is compelled to change that state by forces impressed upon it.*^{[13]}^{: 114 }

Newton's first law expresses the principle of inertia: the natural behavior of a body is to move in a straight line at constant speed. In the absence of outside influences, a body's motion preserves the status quo.

The modern understanding of Newton's first law is that no inertial observer is privileged over any other. The concept of an inertial observer makes quantitative the everyday idea of feeling no effects of motion. For example, a person standing on the ground watching a train go past is an inertial observer. If the observer on the ground sees the train moving smoothly in a straight line at a constant speed, then a passenger sitting on the train will also be an inertial observer: the train passenger *feels* no motion. The principle expressed by Newton's first law is that there is no way to say which inertial observer is "really" moving and which is "really" standing still. One observer's state of rest is another observer's state of uniform motion in a straight line, and no experiment can deem either point of view to be correct or incorrect. There is no absolute standard of rest.^{[note 4]}

### Second

*The change of motion of an object is proportional to the force impressed; and is made in the direction of the straight line in which the force is impressed.*^{[13]}^{: 114 }

By "motion", Newton meant the quantity now called momentum, which depends upon the amount of matter contained in a body, the speed at which that body is moving, and the direction in which it is moving. In modern notation, the momentum of a body is the product of its mass and its velocity:

The forces acting on a body add as vectors, and so the total force on a body depends upon both the magnitudes and the directions of the individual forces. When the net force on a body is equal to zero, then by Newton's second law, the body does not accelerate, and it is said to be in mechanical equilibrium. A state of mechanical equilibrium is *stable* if, when the position of the body is changed slightly, the body remains near that equilibrium. Otherwise, the equilibrium is *unstable.*

A common visual representation of forces acting in concert is the free body diagram, which schematically portrays a body of interest and the forces applied to it by outside influences.^{[17]} For example, a free body diagram of a block sitting upon an inclined plane can illustrate the combination of gravitational force, "normal" force, friction, and string tension.^{[note 5]}

Newton's second law is sometimes presented as a *definition* of force, i.e., a force is that which exists when an inertial observer sees a body accelerating. In order for this to be more than a tautology — acceleration implies force, force implies acceleration — some other statement about force must also be made. For example, an equation detailing the force might be specified, like Newton's law of universal gravitation. By inserting such an expression for into Newton's second law, an equation with predictive power can be written.^{[note 6]} Newton's second law has also been regarded as setting out a research program for physics, establishing that important goals of the subject are to identify the forces present in nature and to catalogue the constituents of matter.^{[note 7]}

### Third

*To every action, there is always opposed an equal reaction; or, the mutual actions of two bodies upon each other are always equal, and directed to contrary parts.*^{[13]}^{: 116 }

Overly brief paraphrases of the third law, like "action equals reaction" might have caused confusion among generations of students: the "action" and "reaction" apply to different bodies. For example, consider a book at rest on a table. The Earth's gravity pulls down upon the book. The "reaction" to that "action" is *not* the support force from the table holding up the book, but the gravitational pull of the book acting on the Earth.^{[note 8]}

Newton's third law relates to a more fundamental principle, the conservation of momentum. The latter remains true even in cases where Newton's statement does not, for instance when force fields as well as material bodies carry momentum, and when momentum is defined properly, in quantum mechanics as well.^{[note 9]} In Newtonian mechanics, if two bodies have momenta and respectively, then the total momentum of the pair is , and the rate of change of is

### Candidates for additional laws

Various sources have proposed elevating other ideas used in classical mechanics to the status of Newton's laws. For example, in Newtonian mechanics, the total mass of a body made by bringing together two smaller bodies is the sum of their individual masses. Frank Wilczek has suggested calling attention to this assumption by designating it "Newton's Zeroth Law".^{[26]} Another candidate for a "zeroth law" is the fact that at any instant, a body reacts to the forces applied to it at that instant.^{[27]} Likewise, the idea that forces add like vectors (or in other words obey the superposition principle), and the idea that forces change the energy of a body, have both been described as a "fourth law".^{[note 10]}

## Work and energy

Physicists developed the concept of energy after Newton's time, but it has become an inseparable part of what is considered "Newtonian" physics. Energy can broadly be classified into kinetic, due to a body's motion, and potential, due to a body's position relative to others. Thermal energy, the energy carried by heat flow, is a type of kinetic energy not associated with the macroscopic motion of objects but instead with the movements of the atoms and molecules of which they are made. According to the work-energy theorem, when a force acts upon a body while that body moves along the line of the force, the force does *work* upon the body, and the amount of work done is equal to the change in the body's kinetic energy.^{[note 11]} In many cases of interest, the net work done by a force when a body moves in a closed loop — starting at a point, moving along some trajectory, and returning to the initial point — is zero. If this is the case, then the force can be written in terms of the gradient of a function called a scalar potential:^{[34]}^{: 303 }

^{[35]}

^{: 19 }The fact that the force can be written in this way can be understood from the conservation of energy. Without friction to dissipate a body's energy into heat, the body's energy will trade between potential and (non-thermal) kinetic forms while the total amount remains constant. Any gain of kinetic energy, which occurs when the net force on the body accelerates it to a higher speed, must be accompanied by a loss of potential energy. So, the net force upon the body is determined by the manner in which the potential energy decreases.

## Examples

### Uniformly accelerated motion

If a body falls from rest near the surface of the Earth, then in the absence of air resistance, it will accelerate at a constant rate. This is known as free fall. The speed attained during free fall is proportional to the elapsed time, and the distance traveled is proportional to the square of the elapsed time.^{[36]} Importantly, the acceleration is the same for all bodies, independently of their mass. This follows from combining Newton's second law of motion with his law of universal gravitation. The latter states that the magnitude of the gravitational force from the Earth upon the body is

If the body is not released from rest but instead launched upwards and/or horizontally with nonzero velocity, then free fall becomes projectile motion.^{[37]} When air resistance can be neglected, projectiles follow parabola-shaped trajectories, because gravity affects the body's vertical motion and not its horizontal. At the peak of the projectile's trajectory, its vertical velocity is zero, but its acceleration is downwards, as it is at all times. Setting the wrong vector equal to zero is a common confusion among physics students.^{[38]}

### Uniform circular motion

When a body is in uniform circular motion, the force on it changes the direction of its motion but not its speed. For a body moving in a circle of radius at a constant speed , its acceleration has a magnitude

^{[note 12]}The force required to sustain this acceleration, called the centripetal force, is therefore also directed toward the center of the circle and has magnitude . Many orbits, such as that of the Moon around the Earth, can be approximated by uniform circular motion. In such cases, the centripetal force is gravity, and by Newton's law of universal gravitation has magnitude , where is the mass of the larger body being orbited. Therefore, the mass of a body can be calculated from observations of another body orbiting around it.

^{[39]}

^{: 130 }

Newton's cannonball is a thought experiment that interpolates between projectile motion and uniform circular motion. A cannonball that is lobbed weakly off the edge of a tall cliff will hit the ground in the same amount of time as if it were dropped from rest, because the force of gravity only affects the cannonball's momentum in the downward direction, and its effect is not diminished by horizontal movement. If the cannonball is launched with a greater initial horizontal velocity, then it will travel farther before it hits the ground, but it will still hit the ground in the same amount of time. However, if the cannonball is launched with an even larger initial velocity, then the curvature of the Earth becomes significant: the ground itself will curve away from the falling cannonball. A very fast cannonball will fall away from the inertial straight-line trajectory at the same rate that the Earth curves away beneath it; in other words, it will be in orbit (imagining that it is not slowed by air resistance or obstacles).^{[40]}

### Harmonic motion

Consider a body of mass able to move along the axis, and suppose an equilibrium point exists at the position . That is, at , the net force upon the body is the zero vector, and by Newton's second law, the body will not accelerate. If the force upon the body is proportional to the displacement from the equilibrium point, and directed to the equilibrium point, then the body will perform simple harmonic motion. Writing the force as , Newton's second law becomes

One reason that the harmonic oscillator is a conceptually important example is that it is good approximation for many systems near a stable mechanical equilibrium.^{[note 13]} For example, a pendulum has a stable equilibrium in the vertical position: if motionless there, it will remain there, and if pushed slightly, it will swing back and forth. Neglecting air resistance and friction in the pivot, the force upon the pendulum is gravity, and Newton's second law becomes

A harmonic oscillator can be *damped,* often by friction or viscous drag, in which case energy bleeds out of the oscillator and the amplitude of the oscillations decreases over time. Also, a harmonic oscillator can be *driven* by an applied force, which can lead to the phenomenon of resonance.^{[41]}

### Objects with variable mass

Newtonian physics treats matter as being neither created nor destroyed, though it may be rearranged. It can be the case that an object of interest gains or loses mass because matter is added to or removed from it. In such a situation, Newton's laws can be applied to the individual pieces of matter, keeping track of which pieces belong to the object of interest over time. For instance, if a rocket of mass , moving at velocity , ejects matter at a velocity relative to the rocket, then

^{[18]}

^{: 139 }

## Rigid-body motion and rotation

A rigid body is an object whose size is too large to neglect and which maintains the same shape over time. In Newtonian mechanics, the motion of a rigid body is often understood by separating it into movement of the body's center of mass and movement around the center of mass.

### Center of mass

Significant aspects of the motion of an extended body can be understood by imagining the mass of that body concentrated to a single point, known as the center of mass. The location of a body's center of mass depends upon how that body's material is distributed. For a collection of pointlike objects with masses at positions , the center of mass is located at

^{[42]}If the total external force is not zero, then the center of mass changes velocity as though it were a point body of mass . This follows from the fact that the internal forces within the collection, the forces that the objects exert upon each other, occur in balanced pairs by Newton's third law. In a system of two bodies with one much more massive than the other, the center of mass will approximately coincide with the location of the more massive body.

^{[15]}

^{: 22–24 }

### Rotational analogues of Newton's laws

When Newton's laws are applied to rotating extended bodies, they lead to new quantities that are analogous to those invoked in the original laws. The analogue of mass is the moment of inertia, the counterpart of momentum is angular momentum, and the counterpart of force is torque.

Angular momentum is calculated with respect to a reference point.^{[43]} If the displacement vector from a reference point to a body is and the body has momentum , then the body's angular momentum with respect to that point is, using the vector cross product,

^{[15]}

^{: 14–15 }The torque can vanish even when the force is non-zero, if the body is located at the reference point () or if the force and the displacement vector are directed along the same line.

The angular momentum of a collection of point masses, and thus of an extended body, is found by adding the contributions from each of the points. This provides a means to characterize a body's rotation about an axis, by adding up the angular momenta of its individual pieces. The result depends on the chosen axis, the shape of the body, and the rate of rotation.^{[15]}^{: 28 }

### Multi-body gravitational system

Newton's law of universal gravitation states that any body attracts any other body along the straight line connecting them. The size of the attracting force is proportional to the product of their masses, and inversely proportional to the square of the distance between them. Finding the shape of the orbits that an inverse-square force law will produce is known as the Kepler problem. The Kepler problem can be solved in multiple ways, including by demonstrating that the Laplace–Runge–Lenz vector is constant,^{[44]} or by applying a duality transformation to a 2-dimensional harmonic oscillator.^{[45]} However it is solved, the result is that orbits will be conic sections, that is, ellipses (including circles), parabolas, or hyperbolas. The eccentricity of the orbit, and thus the type of conic section, is determined by the energy and the angular momentum of the orbiting body. Planets do not have sufficient energy to escape the Sun, and so their orbits are ellipses, to a good approximation; because the planets pull on one another, actual orbits are not exactly conic sections.

If a third mass is added, the Kepler problem becomes the three-body problem, which in general has no exact solution in closed form. That is, there is no way to start from the differential equations implied by Newton's laws and, after a finite sequence of standard mathematical operations, obtain equations that express the three bodies' motions over time.^{[46]}^{[47]} Numerical methods can be applied to obtain useful, albeit approximate, results for the three-body problem.^{[48]} The positions and velocities of the bodies can be stored in variables within a computer's memory; Newton's laws are used to calculate how the velocities will change over a short interval of time, and knowing the velocities, the changes of position over that time interval can be computed. This process is looped to calculate, approximately, the bodies' trajectories. Generally speaking, the shorter the time interval, the more accurate the approximation.^{[49]}

## Chaos and unpredictability

### Nonlinear dynamics

Newton's laws of motion allow the possibility of chaos.^{[50]}^{[51]} That is, qualitatively speaking, physical systems obeying Newton's laws can exhibit sensitive dependence upon their initial conditions: a slight change of the position or velocity of one part of a system can lead to the whole system behaving in a radically different way within a short time. Noteworthy examples include the three-body problem, the double pendulum, dynamical billiards, and the Fermi–Pasta–Ulam–Tsingou problem.

Newton's laws can be applied to fluids by considering a fluid as composed of infinitesimal pieces, each exerting forces upon neighboring pieces. The Euler momentum equation is an expression of Newton's second law adapted to fluid dynamics.^{[52]}^{[53]} A fluid is described by a velocity field, i.e., a function that assigns a velocity vector to each point in space and time. A small object being carried along by the fluid flow can change velocity for two reasons: first, because the velocity field at its position is changing over time, and second, because it moves to a new location where the velocity field has a different value. Consequently, when Newton's second law is applied to an infinitesimal portion of fluid, the acceleration has two terms, a combination known as a *total* or *material* derivative. The mass of an infinitesimal portion depends upon the fluid density, and there is a net force upon it if the fluid pressure varies from one side of it to another. Accordingly, becomes

^{[52]}

### Singularities

It is mathematically possible for a collection of point masses, moving in accord with Newton's laws, to launch some of themselves away so forcefully that they fly off to infinity in a finite time.^{[54]} This unphysical behavior, known as a "noncollision singularity",^{[47]} depends upon the masses being pointlike and able to approach one another arbitrarily closely, as well as the lack of a relativistic speed limit in Newtonian physics.^{[55]}

It is not yet known whether or not the Euler and Navier–Stokes equations exhibit the analogous behavior of initially smooth solutions "blowing up" in finite time. The question of existence and smoothness of Navier–Stokes solutions is one of the Millennium Prize Problems.^{[56]}

## Relation to other formulations of classical physics

Classical mechanics can be mathematically formulated in multiple different ways, other than the "Newtonian" description (which itself, of course, incorporates contributions from others both before and after Newton). The physical content of these different formulations is the same as the Newtonian, but they provide different insights and facilitate different types of calculations. For example, Lagrangian mechanics helps make apparent the connection between symmetries and conservation laws, and it is useful when calculating the motion of constrained bodies, like a mass restricted to move along a curving track or on the surface of a sphere.^{[15]}^{: 48 } Hamiltonian mechanics is convenient for statistical physics,^{[57]}^{[58]}^{: 57 } leads to further insight about symmetry,^{[15]}^{: 251 } and can be developed into sophisticated techniques for perturbation theory.^{[15]}^{: 284 } Due to the breadth of these topics, the discussion here will be confined to concise treatments of how they reformulate Newton's laws of motion.

### Lagrangian

Lagrangian mechanics differs from the Newtonian formulation by considering entire trajectories at once rather than predicting a body's motion at a single instant.^{[15]}^{: 109 } It is traditional in Lagrangian mechanics to denote position with and velocity with . The simplest example is a massive point particle, the Lagrangian for which can be written as the difference between its kinetic and potential energies:

^{[34]}

^{: 485 }Applying the calculus of variations to the task of finding the path yields the Euler–Lagrange equation for the particle,

^{[9]}

^{: 737 }

Landau and Lifshitz argue that the Lagrangian formulation makes the conceptual content of classical mechanics more clear than starting with Newton's laws.^{[21]} Lagrangian mechanics provides a convenient framework in which to prove Noether's theorem, which relates symmetries and conservation laws.^{[59]} The conservation of momentum can be derived by applying Noether's theorem to a Lagrangian for a multi-particle system, and so, Newton's third law is a theorem rather than an assumption.^{[15]}^{: 124 }

### Hamiltonian

In Hamiltonian mechanics, the dynamics of a system are represented by a function called the Hamiltonian, which in many cases of interest is equal to the total energy of the system.^{[9]}^{: 742 } The Hamiltonian is a function of the positions and the momenta of all the bodies making up the system, and it may also depend explicitly upon time. The time derivatives of the position and momentum variables are given by partial derivatives of the Hamiltonian, via Hamilton's equations.^{[15]}^{: 203 } The simplest example is a point mass constrained to move in a straight line, under the effect of a potential. Writing for the position coordinate and for the body's momentum, the Hamiltonian is

^{[50]}

^{[9]}

^{: 742 }

As in the Lagrangian formulation, in Hamiltonian mechanics the conservation of momentum can be derived using Noether's theorem, making Newton's third law an idea that is deduced rather than assumed.^{[15]}^{: 251 }

Among the proposals to reform the standard introductory-physics curriculum is one that teaches the concept of energy before that of force, essentially "introductory Hamiltonian mechanics".^{[60]}^{[61]}

### Hamilton–Jacobi

The Hamilton–Jacobi equation provides yet another formulation of classical mechanics, one which makes it mathematically analogous to wave optics.^{[15]}^{: 284 }^{[62]} This formulation also uses Hamiltonian functions, but in a different way than the formulation described above. The paths taken by bodies or collections of bodies are deduced from a function of positions and time . The Hamiltonian is incorporated into the Hamilton–Jacobi equation, a differential equation for . Bodies move over time in such a way that their trajectories are perpendicular to the surfaces of constant , analogously to how a light ray propagates in the direction perpendicular to its wavefront. This is simplest to express for the case of a single point mass, in which is a function , and the point mass moves in the direction along which changes most steeply. In other words, the momentum of the point mass is the gradient of :

^{[63]}The expression in brackets is a

*total*or

*material*derivative as mentioned above,

^{[64]}in which the first term indicates how the function being differentiated changes over time at a fixed location, and the second term captures how a moving particle will see different values of that function as it travels from place to place:

## Relation to other physical theories

### Thermodynamics and statistical physics

In statistical physics, the kinetic theory of gases applies Newton's laws of motion to large numbers (typically on the order of the Avogadro number) of particles. Kinetic theory can explain, for example, the pressure that a gas exerts upon the container holding it as the aggregate of many impacts of atoms, each imparting a tiny amount of momentum.^{[58]}^{: 62 }

The Langevin equation is a special case of Newton's second law, adapted for the case of describing a small object bombarded stochastically by even smaller ones.^{[65]}^{: 235 } It can be written

^{[66]}

### Electromagnetism

Newton's three laws can be applied to phenomena involving electricity and magnetism, though subtleties and caveats exist.

Coulomb's law for the electric force between two stationary, electrically charged bodies has much the same mathematical form as Newton's law of universal gravitation: the force is proportional to the product of the charges, inversely proportional to the square of the distance between them, and directed along the straight line between them. The Coulomb force that a charge exerts upon a charge is equal in magnitude to the force that exerts upon , and it points in the exact opposite direction. Coulomb's law is thus consistent with Newton's third law.^{[67]}

Electromagnetism treats forces as produced by *fields* acting upon charges. The Lorentz force law provides an expression for the force upon a charged body that can be plugged into Newton's second law in order to calculate its acceleration.^{[68]}^{: 85 } According to the Lorentz force law, a charged body in an electric field experiences a force in the direction of that field, a force proportional to its charge and to the strength of the electric field. In addition, a *moving* charged body in a magnetic field experiences a force that is also proportional to its charge, in a direction perpendicular to both the field and the body's direction of motion. Using the vector cross product,

If the electric field vanishes (), then the force will be perpendicular to the charge's motion, just as in the case of uniform circular motion studied above, and the charge will circle (or more generally move in a helix) around the magnetic field lines at the cyclotron frequency .^{[65]}^{: 222 } Mass spectrometry works by applying electric and/or magnetic fields to moving charges and measuring the resulting acceleration, which by the Lorentz force law yields the mass-to-charge ratio.^{[69]}

Collections of charged bodies do not always obey Newton's third law: there can be a change of one body's momentum without a compensatory change in the momentum of another. The discrepancy is accounted for by momentum carried by the electromagnetic field itself. The momentum per unit volume of the electromagnetic field is proportional to the Poynting vector.^{[70]}^{: 184 }^{[71]}

There is subtle conceptual conflict between electromagnetism and Newton's first law: Maxwell's theory of electromagnetism predicts that electromagnetic waves will travel through empty space at a constant, definite speed. Thus, some inertial observers seemingly have a privileged status over the others, namely those who measure the speed of light and find it to be the value predicted by the Maxwell equations. In other words, light provides an absolute standard for speed, yet the principle of inertia holds that there should be no such standard. This tension is resolved in the theory of special relativity, which revises the notions of *space* and *time* in such a way that all inertial observers will agree upon the speed of light in vacuum.^{[note 14]}

### Special relativity

In special relativity, the rule that Wilczek called "Newton's Zeroth Law" breaks down: the mass of a composite object is not merely the sum of the masses of the individual pieces.^{[74]}^{: 33 } Newton's first law, inertial motion, remains true. A form of Newton's second law, that force is the rate of change of momentum, also holds, as does the conservation of momentum. However, the definition of momentum is modified. Among the consequences of this is the fact that the more quickly a body moves, the harder it is to accelerate, and so, no matter how much force is applied, a body cannot be accelerated to the speed of light. Depending on the problem at hand, momentum in special relativity can be represented as a three-dimensional vector, , where is the body's rest mass and is the Lorentz factor, which depends upon the body's speed. Alternatively, momentum and force can be represented as four-vectors.^{[75]}^{: 107 }

Newtonian mechanics is a good approximation to special relativity when the speeds involved are small compared to that of light.^{[76]}^{: 131 }

### General relativity

General relativity is theory of gravity that advances beyond that of Newton. In general relativity, gravitational force is reimagined as curvature of spacetime. A curved path like an orbit is not the result of a force deflecting a body from an ideal straight-line path, but rather the body's attempt to fall freely through a background that is itself curved by the presence of other masses. A remark by John Archibald Wheeler that has become proverbial among physicists summarizes the theory: "Spacetime tells matter how to move; matter tells spacetime how to curve."^{[77]}^{[78]} Wheeler himself thought of this reciprocal relationship as a modern, generalized form of Newton's third law.^{[77]} The relation between matter distribution and spacetime curvature is given by the Einstein field equations, which require tensor calculus to express.^{[74]}^{: 43 }^{[79]}

The Newtonian theory of gravity is a good approximation to the predictions of general relativity when gravitational effects are weak and objects are moving slowly compared to the speed of light.^{[72]}^{: 327 }^{[80]}

### Quantum mechanics

Quantum mechanics is a theory of physics originally developed in order to understand microscopic phenomena: behavior at the scale of molecules, atoms or subatomic particles. Generally and loosely speaking, the smaller a system is, the more an adequate mathematical model will require understanding quantum effects. The conceptual underpinning of quantum physics is very different from that of classical physics. Instead of thinking about quantities like position, momentum, and energy as properties that an object *has*, one considers what result might *appear* when a measurement of a chosen type is performed. Quantum mechanics allows the physicist to calculate the probability that a chosen measurement will elicit a particular result.^{[81]}^{[82]} The expectation value for a measurement is the average of the possible results it might yield, weighted by their probabilities of occurrence.^{[83]}

The Ehrenfest theorem provides a connection between quantum expectation values and Newton's second law, a connection that is necessarily inexact, as quantum physics is fundamentally different from classical. In quantum physics, position and momentum are represented by mathematical entities known as Hermitian operators, and the Born rule is used to calculate the expectation values of a position measurement or a momentum measurement. These expectation values will generally change over time; that is, depending on the time at which (for example) a position measurement is performed, the probabilities for its different possible outcomes will vary. The Ehrenfest theorem says, roughly speaking, that the equations describing how these expectation values change over time have a form reminiscent of Newton's second law. However, the more pronounced quantum effects are in a given situation, the more difficult it is to derive meaningful conclusions from this resemblance.^{[note 15]}

## History

Isaac Newton (1643–1727), in a 1689 portrait by Godfrey Kneller

Newton's own copy of his

*Principia*, with hand-written corrections for the second edition, in the Wren Library at Trinity College, CambridgeNewton's first and second laws, in Latin, from the original 1687

*Principia Mathematica*

The concepts invoked in Newton's laws of motion — mass, velocity, momentum, force — have predecessors in earlier work, and the content of Newtonian physics was further developed after Newton's time. Newton combined knowledge of celestial motions with the study of events on Earth and showed that one theory of mechanics could encompass both.^{[note 16]}

### Antiquity and medieval background

The subject of physics is often traced back to Aristotle; however, the history of the concepts involved is obscured by multiple factors. An exact correspondence between Aristotelian and modern concepts is not simple to establish: Aristotle did not clearly distinguish what we would call speed and force, and he used the same term for density and viscosity; he conceived of motion as always through a medium, rather than through space. In addition, some concepts often termed "Aristotelian" might better be attributed to his followers and commentators upon him.^{[88]} These commentators found that Aristotelian physics had difficulty explaining projectile motion.^{[note 17]} Aristotle divided motion into two types: "natural" and "violent". The "natural" motion of terrestrial solid matter was to fall downwards, whereas a "violent" motion could push a body sideways. Moreover, in Aristotelian physics, a "violent" motion requires an immediate cause; separated from the cause of its "violent" motion, a body would revert to its "natural" behavior. Yet a javelin continues moving after it leaves the hand of its thrower. Aristotle concluded that the air around the javelin must be imparted with the ability to move the javelin forward. John Philoponus, a Byzantine Greek thinker active during the sixth century, found this absurd: the same medium, air, was somehow responsible both for sustaining motion and for impeding it. If Aristotle's idea were true, Philoponus said, armies would launch weapons by blowing upon them with bellows. Philoponus argued that setting a body into motion imparted a quality, impetus, that would be contained within the body itself. As long as its impetus was sustained, the body would continue to move.^{[90]}^{: 47 } In the following centuries, versions of impetus theory were advanced by individuals including Nur ad-Din al-Bitruji, Avicenna, Abu'l-Barakāt al-Baghdādī, John Buridan, and Albert of Saxony. In retrospect, the idea of impetus can be seen as a forerunner of the modern concept of momentum.^{[note 18]} (The intuition that objects move according to some kind of impetus persists in many students of introductory physics.^{[92]})

### Inertia and the first law

The modern concept of inertia is credited to Galileo. Based on his experiments, Galileo concluded that the "natural" behavior of a moving body was to keep moving, until something else interfered with it. Galileo recognized that in projectile motion, the Earth's gravity affects vertical but not horizontal motion.^{[93]} However, Galileo's idea of inertia was not exactly the one that would be codified into Newton's first law. Galileo thought that a body moving a long distance inertially would follow the curve of the Earth. This idea was corrected by Isaac Beeckman, René Descartes, and Pierre Gassendi, who recognized that inertial motion should be motion in a straight line.^{[94]}

### Force and the second law

Christiaan Huygens, in his *Horologium Oscillatorium* (1673), put forth the hypothesis that "By the action of gravity, whatever its sources, it happens that bodies are moved by a motion composed both of a uniform motion in one direction or another and of a motion downward due to gravity." Newton's second law generalized this hypothesis from gravity to all forces.^{[95]}

One important characteristic of Newtonian physics is that forces can act at a distance without requiring physical contact.^{[note 19]} For example, the Sun and the Earth pull on each other gravitationally, despite being separated by millions of kilometres. This contrasts with the idea, championed by Descartes among others, that the Sun's gravity held planets in orbit by swirling them in a vortex of transparent matter, *aether*.^{[102]} Newton considered aetherial explanations of force but ultimately rejected them.^{[100]} The study of magnetism by William Gilbert and others created a precedent for thinking of *immaterial* forces,^{[100]} and unable to find a quantitatively satisfactory explanation of his law of gravity in terms of an aetherial model, Newton eventually declared, "I feign no hypotheses": whether or not a model like Descartes's vortices could be found to underlie the *Principia*'s theories of motion and gravity, the first grounds for judging them must be the successful predictions they made.^{[103]} And indeed, since Newton's time every attempt at such a model has failed.

### Momentum conservation and the third law

Johannes Kepler suggested that gravitational attractions were reciprocal — that, for example, the Moon pulls on the Earth while the Earth pulls on the Moon — but he did not argue that such pairs are equal and opposite.^{[104]} In his *Principles of Philosophy* (1644), Descartes introduced the idea that during a collision between bodies, a "quantity of motion" remains unchanged. Descartes defined this quantity somewhat imprecisely by adding up the products of the speed and "size" of each body, where "size" for him incorporated both volume and surface area.^{[105]} Moreover, Descartes thought of the universe as a plenum, that is, filled with matter, so all motion required a body to displace a medium as it moved. During the 1650s, Huygens studied collisions between hard spheres and deduced a principle that is now identified as the conservation of momentum.^{[106]}^{[107]} Christopher Wren would later deduce the same rules for elastic collisions that Huygens had, and John Wallis would apply momentum conservation to study inelastic collisions. Newton cited the work of Huygens, Wren, and Wallis to support the validity of his third law.^{[108]}

Newton arrived at his set of three laws incrementally. In a 1684 manuscript written to Huygens, he listed four laws: the principle of inertia, the change of motion by force, a statement about relative motion that would today be called Galilean invariance, and the rule that interactions between bodies do not change the motion of their center of mass. In a later manuscript, Newton added a law of action and reaction, while saying that this law and the law regarding the center of mass implied one another. Newton probably settled on the presentation in the *Principia,* with three primary laws and then other statements reduced to corollaries, during 1685.^{[109]}

### After the *Principia*

Newton expressed his second law by saying that the force on a body is proportional to its change of motion, or momentum. By the time he wrote the *Principia,* he had already developed calculus (which he called "the science of fluxions"), but in the *Principia* he made no explicit use of it, perhaps because he believed geometrical arguments in the tradition of Euclid to be more rigorous.^{[111]}^{: 15 }^{[112]} Consequently, the *Principia* does not express acceleration as the second derivative of position, and so it does not give the second law as . This form of the second law was written (for the special case of constant force) at least as early as 1716, by Jakob Hermann; Leonhard Euler would employ it as a basic premise in the 1740s.^{[113]} Euler pioneered the study of rigid bodies^{[114]} and established the basic theory of fluid dynamics.^{[115]} Pierre-Simon Laplace's five-volume *Traité de mécanique céleste* (1798–1825) forsook geometry and developed mechanics purely through algebraic expressions, while resolving questions that the *Principia* had left open, like a full theory of the tides.^{[116]}

The concept of energy became a key part of Newtonian mechanics in the post-Newton period. Huygens' solution of the collision of hard spheres showed that in that case, not only is momentum conserved, but kinetic energy is as well (or, rather, a quantity that in retrospect we can identify as one-half the total kinetic energy). The question of what is conserved during all other processes, like inelastic collisions and motion slowed by friction, was not resolved until the 19th century. Debates on this topic overlapped with philosophical disputes between the metaphysical views of Newton and Leibniz, and variants of the term "force" were sometimes used to denote what we would call types of energy. For example, in 1742, Émilie du Châtelet wrote, "Dead force consists of a simple tendency to motion: such is that of a spring ready to relax; living force is that which a body has when it is in actual motion." In modern terminology, "dead force" and "living force" correspond to potential energy and kinetic energy respectively.^{[117]} Conservation of energy was not established as a universal principle until it was understood that the energy of mechanical work can be dissipated into heat.^{[118]}^{[119]} With the concept of energy given a solid grounding, Newton's laws could then be derived within formulations of classical mechanics that put energy first, as in the Lagrangian and Hamiltonian formulations described above.

Modern presentations of Newton's laws use the mathematics of vectors, a topic that was not developed until the late 19th and early 20th centuries. Vector algebra, pioneered by Josiah Willard Gibbs and Oliver Heaviside, stemmed from and largely supplanted the earlier system of quaternions invented by William Rowan Hamilton.^{[120]}^{[121]}

## See also

- History of classical mechanics
- List of eponymous laws
- List of equations in classical mechanics
- List of scientific laws named after people
- List of textbooks on classical mechanics and quantum mechanics
- Norton's dome

## Notes

**^**See, for example, Zain.^{[4]}^{: 1-2 }David Tong observes, "A particle is defined to be an object of insignificant size: e.g. an electron, a tennis ball or a planet. Obviously the validity of this statement depends on the context..."^{[5]}**^**Negative acceleration includes both slowing down (when the current velocity is positive) and speeding up (when the current velocity is negative). For this and other points that students have often found difficult, see McDermott et al.^{[8]}**^**The study of mechanics is complicated by the fact that household words like*energy*are used with a technical meaning.^{[10]}Moreover, words which are synonymous in everyday speech are not so in physics:*force*is not the same as*power*or*pressure*, for example, and*mass*has a different meaning than*weight*.^{[11]}^{[12]}^{: 150 }**^**For textbook discussions, see, e.g., Resnick,^{[14]}Frautschi et al.^{[13]}^{: 62–63 }or José and Saletan.^{[15]}^{: 7–9 }Newton himself believed that absolute space and time existed, but that the only measures of space or time accessible to experiment are relative.^{[16]}**^**One textbook observes that a block sliding down an inclined plane is what "some cynics view as the dullest problem in all of physics".^{[18]}^{: 70 }Another quips, "Nobody will ever know how many minds, eager to learn the secrets of the universe, found themselves studying inclined planes and pulleys instead, and decided to switch to some more interesting profession."^{[13]}^{: 173 }**^**See, for example, the discussion in José and Saletan.^{[15]}^{: 9 }Frautschi et al.,^{[13]}^{: 134 }as well as Feynman, Leighton and Sands,^{[19]}^{: 12-1 }argue that the second law is incomplete without a specification of a force by another law, like the law of gravity. Kleppner and Kolenkow argue that the second law is incomplete without the third law: an observer who sees one body accelerate without a matching acceleration of some other body to compensate would conclude, not that a force is acting, but that they are not an inertial observer.^{[18]}^{[20]}Landau and Lifshitz bypass the question by starting with the Lagrangian formalism rather than the Newtonian.^{[21]}**^**See, for example, Frautschi et al.,^{[13]}^{: 134 }as well as Feynman, Leighton and Sands.^{[19]}^{: 12-2 }**^**See, for example, Low and Wilson,^{[22]}Stocklmayer et al.,^{[23]}Hellingman,^{[24]}and Hodanbosi.^{[25]}**^**See, for example, Frautschi et al.^{[13]}^{: 356 }**^**For the former, see Greiner,^{[28]}or Wachter and Hoeber.^{[29]}For the latter, see Tait^{[30]}and Heaviside.^{[31]}**^**Treatments can be found in, e.g., Chabay et al.^{[32]}and McCallum et al.^{[33]}^{: 449 }**^**Among the many textbook explanations of this are Frautschi et al.^{[13]}^{: 104 }and Boas.^{[34]}^{: 287 }**^**Among the many textbook treatments of this point are Hand and Finch^{[35]}^{: 81 }and also Kleppner and Kolenkow.^{[18]}^{: 103 }**^**Discussions can be found in, for example, Frautschi et al.,^{[13]}^{: 215 }Panofsky and Phillips,^{[70]}^{: 272 }Goldstein, Poole and Safko,^{[72]}^{: 277 }and Werner.^{[73]}**^**Details can be found in the textbooks by, e.g., Cohen-Tannoudji et al.^{[84]}^{: 242 }and Peres.^{[85]}^{: 302 }**^**As one physicist writes, "Physical theory is possible because we*are*immersed and included in the whole process – because we can act on objects around us. Our ability to intervene in nature clarifies even the motion of the planets around the sun – masses so great and distances so vast that our roles as participants seem insignificant. Newton was able to transform Kepler's kinematical description of the solar system into a far more powerful dynamical theory because he added concepts from Galileo's experimental methods – force, mass, momentum, and gravitation. The truly external observer will only get as far as Kepler. Dynamical concepts are formulated on the basis of what we can set up, control, and measure."^{[86]}See, for example, Caspar and Hellman.^{[87]}**^**Aristotelian physics also had difficulty explaining buoyancy, a point that Galileo tried to resolve without complete success.^{[89]}**^**Anneliese Maier cautions, "Impetus is neither a force, nor a form of energy, nor momentum in the modern sense; it shares something with all these other concepts, but it is identical with none of them."^{[91]}^{: 79 }**^**Newton himself was an enthusiastic alchemist. John Maynard Keynes called him "the last of the magicians" to describe his place in the transition between protoscience and modern science.^{[96]}^{[97]}The suggestion has been made that alchemy inspired Newton's notion of "action at a distance", i.e., one body exerting a force upon another without being in direct contact.^{[98]}This suggestion enjoyed considerable support among historians of science^{[99]}until a more extensive study of Newton's papers became possible, after which it fell out of favor. However, it does appear that Newton's alchemy influenced his optics, in particular, how he thought about the combination of colors.^{[100]}^{[101]}

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*Physics*affirmed that solid water should have a greater weight than liquid water for the same volume. We know that this statement is incorrect because the density of ice is lower than that of water (hydrogen bonds create an open crystal structure in the solid phase), and for this reason ice can float. [...] The Aristotelian theory of buoyancy affirms that bodies in a fluid are supported by the resistance of the fluid to being divided by the penetrating object, just as a large piece of wood supports an axe striking it or honey supports a spoon. According to this theory, a boat should sink in shallow water more than in high seas, just as an axe can easily penetrate and even break a small piece of wood, but cannot penetrate a large piece.**^**Sorabji, Richard (2010). "John Philoponus".*Philoponus and the Rejection of Aristotelian Science*(2nd ed.). Institute of Classical Studies, University of London. ISBN 978-1-905-67018-5. JSTOR 44216227. OCLC 878730683.**^**Maier, Anneliese (1982). Sargent, Steven D. (ed.).*On the Threshold of Exact Science*. University of Pennsylvania Press. ISBN 978-0-812-27831-6. OCLC 495305340.**^**See, for example:- Eaton, Philip; Vavruska, Kinsey; Willoughby, Shannon (25 April 2019). "Exploring the preinstruction and postinstruction non-Newtonian world views as measured by the Force Concept Inventory".
*Physical Review Physics Education Research*.**15**(1): 010123. Bibcode:2019PRPER..15a0123E. doi:10.1103/PhysRevPhysEducRes.15.010123. ISSN 2469-9896. S2CID 149482566. - Robertson, Amy D.; Goodhew, Lisa M.; Scherr, Rachel E.; Heron, Paula R. L. (March 2021). "Impetus-Like Reasoning as Continuous with Newtonian Physics".
*The Physics Teacher*.**59**(3): 185–188. doi:10.1119/10.0003660. ISSN 0031-921X. S2CID 233803836. - Robertson, Amy D.; Goodhew, Lisa M.; Scherr, Rachel E.; Heron, Paula R. L. (30 March 2021). "University student conceptual resources for understanding forces".
*Physical Review Physics Education Research*.**17**(1): 010121. Bibcode:2021PRPER..17a0121R. doi:10.1103/PhysRevPhysEducRes.17.010121. ISSN 2469-9896. S2CID 243143427.

- Eaton, Philip; Vavruska, Kinsey; Willoughby, Shannon (25 April 2019). "Exploring the preinstruction and postinstruction non-Newtonian world views as measured by the Force Concept Inventory".
**^**Hellman, C. Doris (1955). "Science in the Renaissance: A Survey".*Renaissance News*.**8**(4): 186–200. doi:10.2307/2858681. ISSN 0277-903X. JSTOR 2858681.**^**LoLordo, Antonia (2007).*Pierre Gassendi and the Birth of Early Modern Philosophy*. New York: Cambridge University Press. pp. 175–180. ISBN 978-0-511-34982-9. OCLC 182818133.**^**Pourciau, Bruce (October 2011). "Is Newton's second law really Newton's?".*American Journal of Physics*.**79**(10): 1015–1022. Bibcode:2011AmJPh..79.1015P. doi:10.1119/1.3607433. ISSN 0002-9505.**^**Fara, Patricia (15 August 2003). "Was Newton a Newtonian?".*Science*.**301**(5635): 920. doi:10.1126/science.1088786. ISSN 0036-8075. S2CID 170120455.**^**Higgitt, Rebekah (2015).*Science and Culture in the Nineteenth Century: Recreating Newton*. New York: Taylor & Francis. p. 147. ISBN 978-1-317-31495-0. OCLC 934741893.**^**Dobbs, Betty Jo Teeter (1975).*The Foundations of Newton's Alchemy: Or, "the Hunting of the Greene Lyon"*. Cambridge University Press. pp. 211–212. ISBN 9780521273817. OCLC 1058581988.**^**West, Richard (1980).*Never at Rest*. Cambridge University Press. p. 390. ISBN 9780521231435. OCLC 5677169.- ^
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*Traité de mécanique céleste*from 1799 to 1805, a work collecting in one place all the theoretical and empirical results of the research predicated on Newton's*Principia*. From that time forward, Newtonian science sprang from Laplace's work, not Newton's.**^**Reichenberger, Andrea (June 2018). "Émilie Du Châtelet's interpretation of the laws of motion in the light of 18th century mechanics".*Studies in History and Philosophy of Science Part A*.**69**: 1–11. Bibcode:2018SHPSA..69....1R. doi:10.1016/j.shpsa.2018.01.006. PMID 29857796. S2CID 46923474.**^**Frontali, Clara (September 2014). "History of physical terms: "energy"".*Physics Education*.**49**(5): 564–573. Bibcode:2014PhyEd..49..564F. doi:10.1088/0031-9120/49/5/564. ISSN 0031-9120. S2CID 122097990.**^**Gbur, Greg (10 December 2018). "History of the Conservation of Energy: Booms, Blood, and Beer (Part 1)".*Skulls in the Stars*. Retrieved 7 March 2022. "History of the Conservation of Energy: Booms, Blood, and Beer (Part 2)". 29 December 2018. Retrieved 7 March 2022. "History of the Conservation of Energy: Booms, Blood, and Beer (Part 3)". 25 August 2019. Retrieved 7 March 2022.**^**Silva, Cibelle Celestino; de Andrade Martins, Roberto (September 2002). "Polar and axial vectors versus quaternions".*American Journal of Physics*.**70**(9): 958–963. Bibcode:2002AmJPh..70..958S. doi:10.1119/1.1475326. ISSN 0002-9505.**^**Reich, Karin (1996). "The Emergence of Vector Calculus in Physics: The Early Decades". In Schubring, Gert (ed.).*Hermann Günther Graßmann (1809–1877): Visionary Mathematician, Scientist and Neohumanist Scholar*. Boston Studies in the Philosophy of Science. Vol. 187. Kluwer. pp. 197–210. ISBN 978-9-048-14758-8. OCLC 799299609.

## Further reading

- Chakrabarty, Deepto; Dourmashkin, Peter; Tomasik, Michelle; Frebel, Anna; Vuletic, Vladan (2016). "Classical Mechanics".
*MIT OpenCourseWare*. Retrieved 17 January 2022. - Thomson, W.; Tait, P. G. (1867). "242,
*Newton's laws of motion*".*Treatise on natural philosophy*. Vol. 1.