Foundation course - PHYSICS Lecture 5-2: Force and motion Dynamics of solid bodies ● Acceleration and force ● Newton’s laws of motion ● Some particular forces (normal, weight, tension, friction) Naďa Špačková spackova@physics.muni.cz Dynamics Force ● is an interaction between objects ● is a vector (determined by its magnitude and its direction) ● magnitude is measured in units called newtons (N): 1 N = kg.m.s-2 Essential questions: ● Why objects move ● What can cause an object to accelerate ● What acts on an object and changes its velocity It is a FORCE Free-body diagrams: ● a physical representation of forces acting on the system Dynamics of solid bodies Acceleration is the result of an unbalanced force acting on an object. Ftable on book Fhand on book FEarth’s mass on book Contact and field forces Contact force: ● an object from the external world touches the system and exerts a force on it Field force: ● the force affects the system without touching ● examples: gravitational force, electromagnetic force gravitational force electrostatic force magnetic force Combining forces F2 = 100 N F1 = 100 N Fnet = 0 N F2 = 100 N F1 = 100 N Fnet = 200 N Fnet = 100 N F2 = 200 N F1 = 100 N Net force: the vector sum of all forces acting on the object Equal forces Opposite directions Equal forces Same direction Unequal forces Opposite directions Newton’s first law Fnet=0 ⇒ a=0 a=0 ⇒ v=constant If the net force is zero, then acceleration equals zero. If acceleration is zero, then velocity does not change – it means, the object is at rest or is moving with a constant velocity. Newton’s first law: An object that is at rest will remain at rest, and an object that is moving will continue to move in a straight line with constant speed, if the net force acting on that object is zero. Newton’s first law Law of inertia Inertia = the tendency of an object to resist changes in velocity If the net force is zero, then an object is in equilibrium. An object is in equilibrium if it is moving at a constant velocity (v = 0 is a special case of the constant velocity). Checkpoint question: Which of the six arrangements correctly show the vector addition of forces F1 and F2 to yield the third vector, which is meant to represent their net force Fnet ? (a) (b) (c) (d) (e) (f) F1 F1 F1 F1 F1 F1 F2 F2 F2 F2 F2 F2 Equilibrium ● the object is in equilibrium, when the net force on an object is zero ● the object in equilibrium moves with constant velocity (or is staying at rest) Two forces acting on the object The equilibrant force has the same magnitude and opposite direction as the resultant force The resultant force is a sum of individual forces To put the object in equilibrium, we must add the equilibrant force. FA FB FA FR FE FA + FB = FR FE = -FR Acceleration and force Velocity increases linearly in time → acceleration is constant Applied force: Fgreen < Fred < Fblue The relationship between force and acceleration is linear → application of equation for a straight line: y = kx + b Acceleration and force When the mass increases, a greater force is needed to produce the same acceleration. The slope is reciprocal of the mass. Using the equation for a straight line y = kx we obtain a = Fnet m Newton’s second law Newton’s second law: the acceleration of an object is proportional to the net force and inversely proportional to the mass of the object being accelerated. a = Fnet m ⇒ Fnet= m⋅a Forces are measured in newtons (N): 1 N = 1 kg.m.s-2 Force is a vector (size, direction) If more than one force is acting on an object, it is necessary to determine the net force (as a sum of individual forces). Fnet Fnet F1 F1F2 F2 There are two horizontal forces acting on a block on a frictionless floor. If a third horizontal force F3 also acts on the block, what are the magnitude and direction of F3 when the block is (a) stationary (b) moving to the left with a constant speed of 5 m/s? 3 N 5 N Example: forces Figure show three situations in which one or two forces act on a puck that moves over frictionless ice along an x axis, in one-dimensional motion. The puck’s mass is m = 0.20 kg. Forces F1 and F2 are directed along the axis. In each situation, what is the acceleration of the puck? 4 N 4 N2 N 1 N2 N 30° Example: forces and acceleration Weight An object’s weight is the gravitational force (due to Earth’s mass) experienced by that object: The gravitational acceleration near Earth’s surface is 9.8 m.s-2 Weight is a force, the proper units are newtons (N). Fg = m g = W m … mass of the object g … gravitational acceleration The normal force Fg FN ● term normal means perpendicular direction of the force ● when a body presses against a surface, the surface deforms and pushes on the body with as normal force FN that is perpendicular to the surface FN − Fg = may FN = m g + m ay FN = m(g + ay) If objects are not accelerating, then ay = 0 FN = m g The normal force FH FH Weight Apparent weight ● acceleration of the system is upward, the net force must be upward ● the upward force of the scale must be greater than the downward force of your weight ● the scale reading is greater than your weight Weightlessness – object’s apparent weight is zero Example: force and acceleration An elevator cab that weights 27.8 kN moves upward. What is the tension in the cable if the cab’s speed is: (a) increasing at a rate of 1.22 m/s2 (b) decreasing at a rate of 1.22 m/s2 ? The tension force Body attached to a cord ● the cord pulls on the body with force T directed away from the body and along the cord ● the cord is massless and unstretchable and it exists only as a connection between two objects ● the cord pulls on both bodies with the same force magnitude T Example: inclined planes The mass of the block is 8.5 kg and the angle θ is 30°. Find: (a) the tension in the cord (b) the normal force acting on the block (c) If the cord is cut, find the magnitude of the resulting acceleration of the block. (Assume no friction) Newton’s third law All forces occur in interaction pairs Interaction pair ● a set of two forces that are in opposite directions, have equal magnitudes, and act on different objects ● sometimes called action-reaction pair ● both forces either exist together or not at all Newton’s third law: When two bodies interact, the forces on the bodies from each other are always equal in magnitude and opposite in direction. FA on B =−FB on A Earth table ball FBE FEB Earth table ball FBT FTB The friction force motion Ft The frictional force is parallel to the surface and directed so as to oppose the sliding. Friction is due to bonding between the body and the surface. body surface Friction ⃗Fs⃗F ⃗Fs⃗F ⃗Fd⃗F ⃗Fd⃗F ⃗a ⃗v object at rest moving object F(t) Kinetic friction ● acts on moving objects ● is exerted on one surface by another when the two surfaces rub against each other because one or both surfaces are moving Static friction ● is the force exerted on one surface by another when there is no motion between the two surfaces Kinetic and static friction Normal force [N] Kineticfriction[N] sandpaper rough table highly polished table The slope of the line on a kinetic friction force v. normal force graph is called the coefficient of kinetic friction, μk . Ff ,kinetic=μk FN Ff ,static≤μs FN μs is the coefficient of static friction between the two surfaces The friction forces Ft are always perpendicular to the normal force. A girl, who has a mass of 45 kg, is going down a slide sloped at 27°. The coefficient of kinetic friction is 0.23. How fast does she slide 1.0 s after starting from rest? Example: inclined planes Example: inclined planes +y +x Fg +y +x Fg Fn Ff +y +x Fg Fn Ff Fnet