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Delve into frictional forces, circular motion, and numerical methods in physics, with emphasis on applying Newton’s laws in various scenarios. The chapter covers fundamental forces, field effects, and velocity-dependent forces.
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More applications of Newton’s laws (chapter five) • Forces of friction (static, kinetic) • Uniform circular motion • Nonuniform circular motion • Velocity dependent forces • Numerical methods • Fundamental forces • Gravitational field
Friction • Force acting parallel to an interface that opposes the relative motion • Static – frictional force opposite to applied force - magnitude fs • where s is the coefficient of static friction and n is the magnitude of the normal forces between the surfaces • the equality holds just as the object starts to slip
Friction • Kinetic – frictional force opposite to relative motion – magnitude fk • where k is the coefficient of static friction and n is the magnitude of the normal forces between the surfaces • the kinetic frictional force is constant • s and k are constants that depend on the nature of the surfaces • Usually, s > k
Friction • Note: Static friction is not constant – it is whatever is needed to match the applied force, up to the limit of Sn • As the applied force increases, the static frictional force also increases, until the limit, then the object begins to slide, and the frictional force goes to a constant value
Friction • ConcepTest • Examples • Demo
+y +x m1 m1 m2 m2 Example
Question • What do you call a broken boomerang?
Question • What do you call a broken boomerang? • Answer: A stick.
Newton’s 2nd law applied to uniform circular motion A mass in uniform circular motion (speed v) accelerates according to This acceleration must be caused by some force along a direction towards the center of the radius of curvature (r)
L r Example: conical pendulum
Uniform circular motion • ConcepTest
R Nonuniform circular motion • If an object changes its speed while in circular motion, there is both a radial and a tangential component to the acceleration, therefore, there will be a radial and tangential force applied. • Example: mass moving in a vertical circle
Words of wisdom • "If I had only known, I would have been a locksmith."-Albert Einstein • "There is no clearer manifestation of pure evil than teachers giving assignments over holiday breaks."-James Halloran
Velocity dependent forces Two models: 1. Force proprtional to the velocity (viscous, low speed) b is a constant that depends on the object size and shape and the medium 2. Force proportional to the square of the magnitude of the velocity (air, high speed) D: drag coefficient : density of air A: cross sectional area of object
Velocity dependent forces 1. Force proprtional to the velocity
Velocity dependent forces Can solve differential equation where = m/b is a time constant related to the motion Or, just find terminal speed (a=0)
Velocity dependent forces Force proportional to the square of the magnitude of the velocity Nonlinear differential equation Terminal speed:
Words of wisdom • "I love deadlines. I like the whooshing sound they make as they fly by."-Douglas Adams • "In a survey taken several years ago, all incoming freshman at MIT were asked if they expected to graduate in the top half of their class. Ninety-seven percent responded that they did."-??? • "We made too many wrong mistakes."-Yogi Bera
Numerical representations of particle dynamics Euler method
Fundamental forces of nature Gravitational: force between any two objects where G is the universal gravitational constant Electromagnetic: force between two charged objects (q) where ke is the Coulomb constant Nuclear (strong) – short range Weak – short range
Gravitational field • Field: the effect in a region of space that induces a force on an object • e.g the field (created by a mass) exerts the force on the other masses
Last bad joke for this chapter • An atom walking down the street says to its friend “I think I lost an electron. The friend asks “Are you sure?” to which the first atom repiles “Yea, I’m positive.”