Physics 101 For Perpetual Motion Inventors

Here's a quick review of some of the elementary physics principles most often misapplied. This compilation is obviously not complete. Parts of this may be redundant and even repetitious, but repetition often helps impress important points on the mind. This is a checklist/reminder of things you need to know thoroughly before embarking on analysis of any machine or mechanical system. Consult a good elementary physics book for more details, and for examples.

This document began its life as a review of basic physics for perpetual motion machine inventors, who often misapply elementary physics. For that reason it emphasizes those mechanics principles applicable to machines. However, these are basic to all of physics, and if not properly understood, can adversely affect understanding of everything else in physics.

Mechanics.

Vector quantities are shown in boldface font style.

Scalars and Vectors

• A scalar is a physical quantity whose definition does not in any way depend on direction in space. Scalars include time, mass, volume, temperature, density and others. The size of a scalar quantity is represented as a number. In physical equations, scalars obey the algebra of numbers.

• A vector is a physical quantity dependent on direction in space. A vector has both size and direction, and both must be specified to uniquely characterize the vector. Vector quantities include displacement, velocity, acceleration, momentum, angular momentum and others. Since surface area has spatial orientation, it must often be treated as a vector. Direction matters with vectors. Two vectors are said to be equal only if their sizes and directions are the same.

Sum of three vectors.

• Vectors in physical equations obey an algebra quite different from that of scalar algebra. One useful and intuitive pictorial representation of a vector is an arrow. The length of the arrow represents the vector's size, and the direction of the arrow represents the vector's direction in space. With this representation we may illustrate relations between vectors geometrically.

• The size (or magnitude) of a vector quantity is a scalar, i.e., a number. The size of vector V is symbolized |V|. (Note that the V is boldface, since it is a vector, but the lightface "absolute value" brackets, | |, indicate that the entire quantity is a scalar. I.e., we take the absolute value of a vector, which gives a scalar result.) Alternatively we may simply the vector's letter symbol lightface to indicate that it represents only the size of the vector.

• The sum of two vectors may be found by geometrically placing the arrows representing the vectors head-to tail. The sum may then be found by drawing a new vector from the free tail to the free head.

• The difference between two vectors A - B is found by adding the vectors A and -B where -B is a vector of the same size as B but opposite in direction.

• The projection of a vector onto a line is Vcosq , where q  is the angle between the vector and the line and V is the size of the vector. This may be found geometrically by constructing lines perpendicular to the reference line and from the head and tail of the vector. The length along the reference line lying between the construction lines is the "projection of the vector along that line".

Component of a vector on a line.

• Components of vectors. When dealing with vectors algebraically it's useful to represent a vector by its components. The component of a vector is the projection of that vector onto a chosen coordinate axis. The component of a vector is usually treated as a scalar quantity. While the coordinate axis can be any line, we customarily use the axes of a Cartesian coordinate system, specifying the x, y, and z components of the vector. When this is done, any vector in the space is uniquely defined by specifying the coordinate axes, and the vector's components along those axes, (x,y,z). Sometimes it's even useful to have a set of coordinate axes that are not orthogonal (perpendicular), so long as the axes "span the space" (are able to uniquely represent any vector in the space by its components). This requirement is met if the three axes do not all lie in the same plane and no two are collinear.

Components on Cartesian axes.

• Usually the vectors' tails aren't on a coordinate axis. Drop two perpendiculars to the axis, from the vector's head, and from its tail. Then the component on that axis is the length between the feet of these perpendiculars. The illustration shows vectors lying in an x,y plane, but the same principle is used with three dimensional situations.

• The components of vectors are signed numbers; they may have positive or negative sign. Subtract the tail projection value from the head projection value to get that signed number.

• If the components of two vectors are (x₁,y₁,z₁) and (x₂,y₂,z₂) then the components of the sum of these vectors is (x₁+x₂,y₁+y₂,z₁+z₂).

• The product of a vector and a scalar, Vs, is a vector of size |V|s. It has the same direction as V.

• Two kinds of vector products are useful in physics, and these will be defined later when we need them.

Kinematics

• Physical quantities of different kinds are distinguished by unit and dimension labels. These two terms are not synonyms. See my glossary of physics terms. Quantities with different dimensions are never added. Quantities with different units are never added. Vector and scalar quantities cannot be added together.

• Fundamental measurables are those that are not defined by equations, but defined by specifying a measurement procedure to determine their size. They are scalar quantities. Length, mass, and time are the three fundamental measurables of mechanics. In study of thermal physics, optics and electricity, additional fundamental measurements are used.

• Displacement is the vector representing the relative position of two points in space. Its size is the distance between the points; its direction is the direction of the line segment joining the points. When we speak of displacement of a body during a time interval, the displacement is a vector drawn from the earlier (initial) position to the later (final) position of that body.

• The velocity of a body is defined as v = Dx/ Dt, where Dx is the displacement during the infinitesimal time interval Dt.

• The acceleration of a body is defined as a = Dv/ Dt, where Dv is the instantaneous velocity during the infinitesimal time interval Dt.

Statics

• A static system is one in which all parts of a system are at rest relative to an inertial frame of reference. Statics is the physics of such systems.

  Finding the torque due to a force on a body.

• Torque expresses the ability of force to cause rotation of a body about a chosen particular axis of rotation. While torque is a vector quantity, it may be treated as a signed scalar when all the forces of concern lie in a common plane, as is the case with rotating wheels. The figure shows such a body, of arbitrary shape. We wish to know whether the effect of force F to cause rotation about the axis marked X labeled "Center of torques". P is the point of application of force on the body. Extend a "line of action" along the force vector far enough to allow drawing a line perpendicular to it and passing through the center of torques. The length of this last line (L) is called the "lever arm" of the force. The size of the torque about this center of torques is then FL. If the force is such that it alone would rotate the body clockwise around the center of torques, we assign it a negative sign. If it alone would rotate the body counter-clockwise, we assign it a positive sign.

• The torque concept is useful in both static and dynamic systems, but in static systems nothing rotates, so the net torque on each part of the system is zero.

• When the forces on a body do not lie in a single plane, we must treat torque as a vector. The definition is as above in the plane that contains the vector and the chosen center of torques. The vector representing the torque is along a line perpendicular to that plane and passing through the center of torques. If, as you look at this plane, the torque would produce clockwise rotation, then the torque vector is pointing toward you. If the torque would produce counter-clockwise rotation, the torque vector points away from you. The right hand rule is a useful mnemonic for getting this right. Curl your fingers around the line of the torque, with your fingers curling in the direction of the rotation, then your thumb points in the direction of the torque.

• When a body is at rest, the net force on the body is zero and the net torque on the body is also zero. Furthermore, the net torque on the body is zero no matter what center of torques is chosen. That simply means that the body does not rotate about any axis. It isn't rotating at all.

• Putting this another way: If the net torque on a body is zero about an axis, it will also be zero about any other chosen axis, even an axis that does not even pass through the body.

• The center of mass of an extended body is an imaginary (but useful) point defined this way. It is the point through which any plane you draw will split the body into two parts of equal mass.

• The center of gravity of an extended body is that point through which any plane you draw will split the body into two parts of equal weight in a gravitational field.

Dynamics

• Mass is an intrinsic property of a body. Gravitational mass is measured by determining the gravitational force on a body relative to a mass standard. Inertial mass is determined and defined by Newton's third second law (see below). So far as we know, gravitational and inertial mass are the same.

• An inertial frame of reference (coordinate system) is one that isn't accelerating. That means the reference frame is either at rest or moving with constant velocity. More specifically, an inertial frame is a system in which Newton's law F = ma applies, where F is the sum of all real forces acting on the body of mass m (see below).

• Dynamics is the study of systems in which some parts of the system accelerate. Newton's F = ma applies to each part of such systems.

• For our present purposes, we define real forces to be of two kinds: (a) forces at points where bodies contact, due to elastic deformation, (b) gravitational, electric, magnetic and nuclear forces that can act on bodies that aren't in contact (acting "at a distance"). The term "real force" does not include fictitious forces, which are useful when doing problems in accelerated coordinate systems. Fictitious forces include centrifugal and Coriolis forces.

• The net force on a body is the vector sum of all real forces acting on that body, and no other forces. This statement assumes the problem is being done in an inertial frame of reference.

• If F is the net real force on a body and a is the acceleration of the center of mass of that body. Then F = ma. (Newton's first and second laws in the special case where the mass doesn't change.)

• When the net force on a body is zero: (1) A body at rest will remain at rest. (2) A moving body continues to with constant speed in a straight line. This Newton's first law.

• Newton's first two laws are embodied in this more general statement: The rate of change of momentum of a body is proportional to the net force acting on it. In equation form, F = d(mv)/dt. This is a vector equation, and applies even in those cases where the mass may change size.

• Newton's third law: If body A exerts a force on body B, then B exerts an equal size and oppositely directed force on A. It can be written: F_AB = - F_BA. Remember that forces are vectors. The two forces of Newton's third law act on different bodies.

• To avoid errors in application of Newton's laws (above) it helps to mentally "isolate each part of the system" then tally all real forces acting on that part of the system (and only that part) before applying Newton's F = ma to it. Many forces acting on one part of the system are due to contact with other parts of the system (or to "action at a distance" forces). Newton's third law applies to them, but one must be careful not to add forces acting on other parts when summing the forces on one part. Newton's laws apply to each part of the system, any grouping of parts, or the entire system.

• When several parts of a system are grouped together as a single 'system' for the purpose of applying Newton's second law, the net force on that system need not include any of the internal forces within the system, since they sum to zero according to Newton's third law. Some books write Newton's second law for a system of mass m as F_{net, external} = ma for this reason.

• Friction acts in a direction to oppose slipping or sliding motion of the bodies at their contact surface. Forces due to friction are tangent to the contact surface where the bodies touch. Note: The short phrase "friction opposes motion" should not be used for it can be misleading. The force due to friction exerted by the floor on your feet acts in the direction of your walking motion. This force due to friction on your feet helps prevent your feet slipping backward as they might on ice. The force due to friction of the pavement acting on your automobile's wheels is forward, in the direction of the auto's motion. Forces due to friction and forces due to rolling resistance are the only forces that sustain your car's forward motion. Friction relates to two surfaces either at rest or sliding. Rolling resistance is quite another matter. See next item.

• Rolling resistance results from elastic or non-elastic deformations of bodies in contact, even if they are not slipping or sliding. To illustrate the difference between rolling resistance and friction, consider this example. A ball or cylinder rolls on an infinite horizontal plane. Will it roll forever? No. Why?
  • Not simply because of friction. Friction is, by definition, a force acting tangent to the surface. Friction would act parallel to the plane in this situation.
  • If such a tangential force acted opposite to the motion of the ball, this would decrease the ball's forward velocity, but it would have a torque that would be in a direction to increase the angular velocity of the ball. This is contradictory.
  • If a tangential force were in a direction to decrease the angular velocity it would have a torque that would increase the forward linear velocity. Likewise contradictory.
  But elastic forces associated with deformations at the contact surface are not parallel to the plane, and they may not be quite perpendicular to the plane. They can provide the torque in the correct sense to slow the ball's rotation provide the vertical force to balance the weight, and a horizontal force to slow the forward motion of the center of mass.

• Both friction and rolling resistance are usually present where two bodies are in contact. We sometimes carelessly combine their effects and call it "friction". Sometimes we can get by with that without introducing errors, but we should be more careful. See next item.

• Two bodies that are in frictionless contact and do not deform at the points of contact exert forces on each other that are normal (perpendicular) to the surfaces at the point of contact. This also applies to frictionless rollers and ball bearings. (However, if the surfaces deform, there can be tangential force components of "rolling resistance" even in the frictionless case.)

• All materials deform somewhat under load. Perfectly rigid bodies are impossible in nature, for if they collided, reaction forces at the point of contact would be infinite in size and of infinitesimal duration.

• When the net torque on a body is zero: (1) A body that is not rotating will continue without rotation. (2) A body that is rotating will continue rotating with the same angular speed.

• If the net (total) force on a body has zero component in one direction, the body will not move in that direction.

• If the vector sum of all forces and the sum of all torques acting on a body is zero then that body is not accelerating.

• The work done by a force acting on a body is the product of the force's component in the direction of motion multiplied by the distance the body moves in that direction. If a force is perpendicular to the direction of motion, that force does no work on the body. If a force acts on a body, and there's no motion of the body, that force does no work. Work is a scalar quantity.

• A closed system is one in on which no outside forces act. Since no system is perfectly closed we relax this a bit. If none of the external forces acting on the system affect it significantly, we may treat it as closed. If we can determine (measure or predict) the effect of an external force on the system we can separate that effect from the others we are interested in or "correct" for it.

• Usually when we use the term "component of a vector" we are talking about a scalar, the projection of the vector onto a line. But sometimes it's useful to speak of "vector components of a vector". The vector components of a vector V are any set of vectors that sum to that vector V. The vector components of a vector V acting together are physically equivalent to the single vector V. In motion problems with complicated paths, it's useful to speak of a vector's radial and tangential components.

• The momentum of a body is the product of its mass and velocity, and is therefore a vector quantity. P = mv.

• Conservation of momentum. The net momentum of the parts of a closed system remains constant, no matter what's going on within the system. This follows from Newton's third law.

• The centripetal force acting on a rotating body is simply the radial component of the net force acting on that body. The radial component of a force is the vector component in the direction of a line drawn from the body to the center of rotation. The centripetal force is not a "new" force to be added to the real forces when finding the net force. Nor is it a fictitious force. It is a real vector component of real forces. We are here assuming the analysis is being carried out in an inertial coordinate system. In advanced courses one sometimes does such problems in a rotating coordinate system. Such systems are non-inertial, so Newton's second law for real forces does not apply. However, if one introduces "fictitious" forces such as the centrifugal force, Coriolis force, etc. into the sum of forces, one can use F = ma. This neat trick is not recommended for beginners.

• All material bodies are at least somewhat deformable.

• No physical influence can propagate through space between two different points instantaneously. (Nothing can be in different places at the same time.)

Gravity, energy.

• Newton's law of gravitation. Two spherical bodies of masses m₁ and m₂ whose centers are a distance r apart exert forces of attraction on each other of size F = Gm₁m₂/r². G is the universal gravitational constant.

• Gravitational potential energy is a convenient concept when dealing with bodies or systems in a gravitational field. It allows one to treat the body as "possessing" energy due to its position in the field, thereby avoiding the need for including the gravitational source as part of the system. The gravitational potential energy of a body at a certain position is just the work that must be done on the body to move it to that position from some fixed reference position. Gravitational potential is the potential energy of a body divided by the mass of the body.

• The work done in moving a body from point A to B in a gravitational field is independent of the path along which it moves between A and B. The potential energy difference between those points is independent of the path. It follows that the potential energy change around any closed loop path is zero. These characterize the field as energy conservative.

• Conservation of Energy. Energy can be present in many forms: kinetic, thermal, nuclear, various kinds of potential energy and others. But when all forms are accounted for and measured, the total energy of a closed system remains constant.

Liquids, hydrostatics.

These principles apply only to static systems, where nothing in the system is moving. Some of them (those that mention "level" or "height") implicitly assume an experiment done on earth, or in a gravitational field where these words have specific meaning with respect to the direction of the field.

• Solids undisturbed preserve their shape. Liquids flow to conform to the shape of their container. Solids have rigidity and elasticity, but can be deformed by compression, stretching and shear. Most liquids strongly resist being compressed, and to a first approximation may be considered to maintain constant volume over a wide range of pressures.

• Liquids seek their own level. More precisely, any two connectable points on the surface of a liquid at rest are at the same height.

• Liquid pressure is a scalar quantity. Liquid contacting a solid surface is responsible for a force on that surface. The force is perpendicular to the surface and of size F = PA where P is the liquid pressure and A is the area of the surface. The area must be small enough that the pressure is essentially constant over the surface. This is in fact the definition of pressure, which is, in calculus form, P = dF/dA.

• Pressure at a given point in a liquid exerts force on an infinitesimal area at that point, which is the same size no matter what the orientation of that area. This is often abbreviated in a potentially misleading slogan "Pressure acts equally in all directions."

  A continuous line may be drawn through the liquid, connecting points A and B. Therefore the pressure difference between these points is r gH, where r is the liquid density.

• Any two connectable points in a liquid are at the same pressure if they are at the same height.

• The pressure difference between two connectable points in a liquid is r gH. r  is the liquid density, g is the acceleration due to gravity and H is the height difference between the two points.

• Pascal's principle. If the pressure changes at one point in a liquid, it changes by the same amount at all other points connectable to that point.

• Archimedes' principle. If a body is floating on or immersed in a liquid, the liquid exerts a net upward "buoyant" force due to the pressure differences on its surfaces. Horizontal forces due to pressure add to zero, but vertical components don't because of height differences. Using the principles above, one can derive a simple result: The buoyant force on the object is equal to the weight of the liquid the object has displaced. Warning: There must be liquid underneath the body for there to be an upward buoyant force on it. The buoyant force is due to pressure differences; it isn't the result of the "desire" of the water displaced (pushed aside) to return to its original place.

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