simple harmonic motion. starter make a list of objects that experience vibrations:
DESCRIPTION
PERIODIC MOTION PERIODIC MOTION: Any motion that repeats itself precisely over equal periods of time. If that periodic motion is generated by a linear restoring force it is SIMPLE HARMONIC MOTION.TRANSCRIPT
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SIMPLE HARMONIC MOTION
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STARTER
• MAKE A LIST OF OBJECTS THAT EXPERIENCE VIBRATIONS:
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PERIODIC MOTION
• PERIODIC MOTION: Any motion that repeats itself precisely over equal periods of time.
• If that periodic motion is generated by a linear restoring force it is SIMPLE HARMONIC MOTION.
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HOOKE’s LAW• Recall Hooke’s Law:
F= -kx• x is the amount of extension or compression of
a spring• Spring constant, k , describes the force
necessary to stretch or compress an individual spring. Each spring is different.
• the negative sign indicates that the force always opposes the direction of the stretch, “restoring” the object to its rest or equilibrium position
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Quantities that Describe Periodic Motion
• Period: the length of time required to complete one full cycle of motion
• Frequency: the number of cycles in a given time
• Period and frequency are inversely related
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ENERGYET= ½ mv2 + ½ kx2
• x is the position• At the ends of the
oscillation the mass stops and changes direction, so all of the energy is elastic potential energy
• At equilibrium (x=0) the string is not stretched so all energy is kinetic.
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VELOCITYv = vmax √ 1- x2/A2
• v is the speed of the mass at any position of its motion
• x is any position• A is maximum amplitude• vmax is the maximum
speed; occurs at equilibrium position
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UNIFORM CIRCULAR MOTION
• The amplitude of SHM is equal to the radius of Uniform Circular Motion
• Use the UCM equations to describe SHM:a = 4π2A/T2
vmax = 2πA/ T Or T = 2πA/ vmax
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PERIOD and FREQUENCY of mass on spring
• Another arrangement for vmax
vmax2 = k/m A2
• Substituting into UCM equationT = 2π√m/k
• Equation for frequencyf = 1/2π √k/m
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PENDULUM
T =2π √ l /g• l is the length of the pendulum string• g is acceleration due to gravity• This equation is valid for the period of a
pendulum for small angles