From last time Defined mass m and inertia: Defined momentum p:

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Presentation transcript:

From last time Defined mass m and inertia: Defined momentum p: Mass is amount of inertia of a body Measured in kg Defined momentum p: p=mv, momentum is said to be conserved Defined force F: Something that changes a body’s velocity Can transfer momentum from one body to another Started exploring the meaning of these concepts using Newton’s Laws Physics 107, Fall 2006

Mass Define mass to be ‘the amount of inertia of an object’. Can also say mass characterizes the amount of matter in an object. Symbol for mass usually m Unit of mass is the kilogram (kg). Said before that Find experimentally that Physics 107, Fall 2006

Force, weight, and mass 1 Newton = force required to accelerate a 1 kg mass at 1 m/s2. But then what is weight? Weight is a force, measured in Newton’s It is the net force of gravity on a body. F=mg, g=F/m Physics 107, Fall 2006

Is ‘pounds’ really weight? In the English system (feet, pounds, seconds), pounds are a measure of force. So it is correct to say my weight is 170 pounds. Then what is my mass? slugs!! Physics 107, Fall 2006

Momentum conservation We said before that an impressed force changes the momentum of an object. We also said that momentum is conserved. This means the momentum of the object applying the force must have decreased. According to Newton, there must be some force acting on that object to cause the momentum change. Physics 107, Fall 2006

Newton’s third law This is the basis for Newton’s third law: To every action there is always opposed an equal reaction. This is momentum conservation in the language of forces. Physics 107, Fall 2006

Newton’s laws 1st law: Law of inertia Every object continues in its state of rest, or uniform motion in a straight line, unless acted upon by a force. 2nd law: F=ma, or a=F/m The acceleration of a body along a direction is proportional to the total force along that direction, and inversely the mass of the body 3rd law: Action and reaction For every action there is an equal an opposite reaction. Physics 107, Fall 2006

Example: More than one force M=10 kg, F1=200 N Find a a = Fnet/M = 200N/10kg = 20 m/s2 M=10 kg F1=200 N F2 = 100 N Find a M F1 F2 a = Fnet/M = (200N-100N)/10kg = 10 m/s2 Physics 107, Fall 2006

Colliding balls again Before collision: 1 2 During collision 1 2 Force on ball 2 accelerates it Force on ball 1 decelerates it to zero velocity After collision: 1 2 Physics 107, Fall 2006

Balancing forces Force of gravity acts downward on the block. But since the block is not accelerating. The net (total) force must be zero. Another force is present, which balances the gravitational force. It is exerted by the table, on the block. Force of table on block Force of gravity on block Physics 107, Fall 2006

How can the table exert a force? The interaction between the table and the block is a microscopic one. Physics 107, Fall 2006

Force of table on block The table can compress, bend, and flex by distorting the atomic positions. The atomic bond is like a spring and it exerts a force on the block. All forces arise at the atomic (or smaller) scale. Physics 107, Fall 2006

3rd law: Law of force pairs Every force is an interaction between two objects Each of the bodies exerts a force on the other. The forces are equal and opposite An action reaction pair. Force on the block by you Force by the block on you Explain on board why the block moves, but you (and the earth) do not. (Combined with the earth, you are much more massive than the block). and the earth! Physics 107, Fall 2006

Identifying forces If horse exerts force on cart, and cart exerts equal and opposite force on horse, how can the horse and cart move? Physics 107, Fall 2006

Keep the forces straight! For motion of cart, need to identify the net force on the cart. Net horizontal force is force from horse, combined with frictional force of wheels. Physics 107, Fall 2006

How can a car move? Vertical forces Horizontal forces Gravitational force on car Force exerted by road on car Rolling resistance by road on tires Drive Force by road on tires Wheels push push backward against the road, Road pushes forward on the tire Physics 107, Fall 2006

Rockets I apply a force to a ball for a short time t to get it to move. During that time, the ball exerts an equal and opposite force on me! The forces cause the ball and I to move in opposite directions Throw medicine ball on rollerblades Physics 107, Fall 2006

Why did the ball and I move? The forces resulted in accelerations during the short time t Me Ball My acceleration is smaller since my mass is much larger. The acceleration changes my velocity. Shoot CO2 fire extinguishers on roller blades (try two this time - wear helmet!) Physics 107, Fall 2006

Another explanation Before the throw, both the ball and I have zero momentum. So the total momentum is zero. The total momentum is conserved, so after the throw the momenta must cancel (my momentum) + (ball momentum) = 0 (my mass) x (my velocity) = — (ball mass) x (ball velocity) Physics 107, Fall 2006

Gravitational force These forces are equal and opposite, Gravitational force on apple by earth Gravitational force on Earth by apple These forces are equal and opposite, But mearth=6x1024 kg mapple=1 kg Physics 107, Fall 2006

Equal accelerations If more massive bodies accelerate more slowly with the same force… … why do all bodies fall the same, independent of mass? Gravitational force on a body depends on its mass: Therefore acceleration is independent of mass: Physics 107, Fall 2006

A fortunate coincidence A force exactly proportional to mass, so that everything cancels nicely. But a bit unusual. Einstein threw out the gravitational force entirely, attributing the observed acceleration to a distortion of space-time. Physics 107, Fall 2006