Chapter 4: Forces and Laws of Motion Physics 1-2 Richwoods High School Mr. Chumbley Section 1: Changes in Motion Force Forces describe the interactions between an object and its environment A force is an action exerted on an object that may change the object’s state of rest or motion Forces cause a change in motion in three ways: Start moving Stop moving Change direction Measuring Force Forces are measured in different ways depending on the system of measure The SI unit of measure is the newton (N) System SI Mass kg Acceleration m/s2 cgs g cm/s2 Avoirdupois slug ft/s2 Force kg·m/s2= N g·m/s2= dyne lb =slug·ft/s2 How Forces Act Contact Forces Field Forces Pushes or pulls that result Pushes or pulls that do not from direct physical contact between objects Typically called mechanical forces require direct physical contact between objects Examples: Electric Force Magnetic Force Gravitation Force Force Diagrams Force is a vector quantity, so it can be depicted graphically by drawing vectors To help identify the comparative effect of forces acting on an object, drawing a diagram is beneficial A free-body diagram is a graphical representation of a body depicting all forces being exerted on that body Drawing Free-Body Diagrams Only the forces acting on the object are included Any forces exerted by the object are excluded When drawing a force vector in a free-body diagram, label it clearly with either a symbol or the magnitude of the force Free-body diagrams are often very simplified pictures showing Sample Problem A The picture below shows a little girl pulling a dog in a sled. Draw a free-body diagram for this sled. Assume the magnitudes of the forces acting on the sled are 60N by the string, 130 N by the earth, and 90 N upward by the ground. The string exerts 60N in the direction the string pulls Earth exerts a downward force of 130 N on the sled The ground exerts an upward force of 90 N on the sled Fground Fstring Fgravity Homework P. 122 Practice A #1-2 Section 1 Formative Assessment #5 Section 2: Newton’s First Law Newton’s Laws of Motion In 1687, Isaac Newton published a work entitled Philosophiæ Naturalis Principia Mathematica In Principia, Newton outlined three laws of motion that became the foundation for describing motion Newton’s First Law Lex I: Corpus omne perseverare in statu suo quiescendi vel movendi uniformiter in directum, nisi quatenus a viribus impressis cogitur statum illum mutare. An object at rest will remain at rest unless acted upon by an external and unbalanced force . An object in motion will remain in motion unless acted upon by an external and unbalanced force. Inertia This law is often times referred to as the Law of Inertia Inertia is the tendency of an object to resist being moved or, if the object is moving, to resist a change in speed or direction Mass is a measure of inertia The more massive an object, the more inertia it posesses Net Force When looking at all of the forces acting on objects, it can be difficult to determine which one is affecting the motion The reality is that all of the forces acting on an object affect its motion, but we can typically simplify all of the forces into a single summative force Net force is a single force whose external effects on a body are the same as the effects of several actual forces acting on the body Net force is the vector sum of all forces acting on an object Sample Problem Four forces act on a hot air balloon, as shown below. Find the magnitude and direction of the net force. 5120 N 1520 N 950 N 4050 N Homework Practice B (p. 126) #1-3 Equilibrium Equilibrium is the state in which the net force on an object is zero Section 3: Newton’s Second and Third Laws Newton’s Second Law Lex II: Mutationem motus proportionalem esse vi motrici impressae, et fieri secundum lineam rectam qua vis illa imprimitur. The acceleration of an object is directly proportional to the net force acting on an object and inversely proportional to the object’s mass. 𝐧𝐞𝐭 𝐟𝐨𝐫𝐜𝐞 = 𝐦𝐚𝐬𝐬 × 𝐚𝐜𝐜𝐞𝐥𝐞𝐫𝐚𝐭𝐢𝐨𝐧 Σ𝐅 = 𝑚𝐚 Sample Problem C (p.129) Roberto and Laura are studying across from each other at a wide table. Laura slides a 2.2 kg book toward Roberto. If the net force acting on the book is 1.6 N to the right, what is the book’s acceleration? Σ𝐅 = 1.6 N 𝑚 = 2.2 kg Σ𝐅 = 𝑚𝐚 ΣF 1.6 N Σ𝐅 𝐚= 𝑚 1.6 N 𝐚= 2.2 kg 𝐚 = 0.73 m s2 to the right Newton’s Third Law Lex III: Actioni contrariam semper et æqualem esse reactionem: sive corporum duorum actiones in se mutuo semper esse æquales et in partes contrarias dirigi. If two objects interact, the magnitude of the force exerted on the first object by the second is equal in magnitude and opposite in direction of the force simultaneously exerted on the second object by the first Action-Reaction Pairs When examining action-reaction pairs, there are a couple key points to understand Action-reaction forces occur simultaneously, not sequentially Action-reaction forces act on different objects All forces exist in pairs Homework: Practice C (p. 130) #1-5 Sample Problem Four forces act on a hot air balloon, as shown below. Find the acceleration of the hot air balloon. 5120 N 1520 N 950 N 4050 N Section 4: Everyday Forces Weight and Normal Force Weight (mg) is a measure of the gravitational force exerted on an object by another much larger object Mass is an inherent property of matter, weight is not Normal force (FN) is a force that acts on a surface in a direction perpendicular to the surface Normal force is often times the reactive force to weight, but it is not Friction In general, any force that opposes motion due to interaction with the environment can be considered friction Static friction is the force that resists the initiation of sliding motion between two objects that are in contact and at rest Kinetic friction is the force that opposes the movement of two surfaces that are in contact and sliding over each other Friction A coefficient of friction is a ratio of the magnitude of the force of friction between two objects in contact to the magnitude of the normal force with which the objects press against each other 𝐹𝑓 = 𝜇𝐹𝑁 For static friction, μs is used 𝐹𝑓 ≥ 𝜇𝑠𝐹𝑁 For kinetic friction, μs is used 𝐹𝑓 = 𝜇𝑘𝐹𝑁 Sample Problem D (p.137) A 24 kg crate initially at rest on a horizontal floor requires 75 N of horizontal force to set it in motion. Find the coefficient of static friction between the crate and the floor. FN = mg 𝐹𝑓 = 𝜇𝑠𝐹𝑁 𝐹𝑓 𝜇𝑠 = 𝐹𝑁 𝜇𝑠 = 75 N = 0.32 2 (24 kg)(9.8 m s ) Ff = 75 N Fa = 75 N mg Sample Problem E (p.138) A student attaches a rope to a 20.0 kg box of books. He pulls with a force of 90.0 N at an angle of 30.0˚ above the horizontal. The coefficient of kinetic friction between the box and the sidewalk is 0.500. Find the acceleration of the box. FN Fa = 90 N 30.0˚ Ff mg Homework: Practice D (p. 137) #1-2 Practice E (p. 139) #1, 4 Sample Problem B (p.125) Derek leaves his physics book on top of a drafting table that is inclined at a 35˚ angle. If the book has a mass of 2.25 kg, what is the coefficient of friction if it remains at rest? FN y Ff x Fg
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