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Do now!
Can you hand your SHM questions in please?
This lesson
• Considering energy changes during SHM• Applying Ek = ½mω2(xo
2 – x2)
ET = ½mω2xo2
Ep = ½mω2x2
where ω = 2πf = 2π/T
S.H.M.Where is the kinetic energy maxiumum?
Where is the potential energy maximum?
It can be shown that….
Ek = ½mω2(xo2 – x2)
ET = ½mω2xo2
Ep = ½mω2x2
where ω = 2πf = 2π/T
Example
A mass-spring system oscillates with an amplitude of 3.5cm. If the force constant of the spring of 250Nm-1 and the mass is 0.5kg, determine(a) the total energy of the system,(b) the maximum speed of the mass(c) the maximum acceleration
• A mass-spring system oscillates with an amplitude of 3.5cm. If the force constant of the spring of 250Nm-1 and the mass is 0.5kg, determine(a) the total energy of the system,(b) the maximum speed of the mass(c) the maximum acceleration
(a) We have m = 0.5kg, xo = 0.035m, k = 250 N/m
= √k/m = √500 = 22.36 rad.s-1
ET = ½mω2xo2 = ½(0.5)(22.36)2(0.035)2 = 0.153J.
• A mass-spring system oscillates with an amplitude of 3.5cm. If the force constant of the spring of 250Nm-1 and the mass is 0.5kg, determine(a) the total energy of the system,(b) the maximum speed of the mass(c) the maximum acceleration
(b) Maximum speed when x = 0 (Ek = max)
At this point, the total energy is all kinetic
Ek = 0.153 J = ½mv2
v2 = (2 x 0.153)/0.5 = 0.612v = 0.78m.s-1
• A mass-spring system oscillates with an amplitude of 3.5cm. If the force constant of the spring of 250Nm-1 and the mass is 0.5kg, determine(a) the total energy of the system,(b) the maximum speed of the mass(c) the maximum acceleration
(c) Maximum acceleration (force) when x = xo
F = -kx = -250 x 0.035 = 8.75 N
a = F/m = 8.75/0.5 = 17.5 m.s-2
Last lesson
• Considering energy changes during SHM• Applying Ek = ½mω2(xo
2 – x2)
ET = ½mω2xo2
Ep = ½mω2x2
where ω = 2πf = 2π/T
This lesson
• Know what is meant by damping• Describe damped oscillations• Know what is meant by natural frequency
and forced oscillation• Describe graphically forced oscillations
near the natural frequency• Know what is meant by resonance and
describe examples
Damping
Damping
In most real oscillating systems energy is lost through friction.
The amplitude of oscillations gradually decreases until they reach zero. This is called damping
Heavy Damping
Sometimes the damping is so large that the motion no longer resembles SHM
Overdamped
The system takes a long time to reach equilibrium
Underdamped
The system makes several oscillations before coming to rest
Critical damping
Equilibrium is reached in the quickest time
Forced vibrations - resonance
YouTube - Tacoma Bridge Disaster
Natural frequency
All objects have a natural frequency that they prefer to vibrate at.
Forced vibrations
If a force is applied at a different frequency to the natural frequency we get forced vibrations
Resonance
If the frequency of the external force is equal to the natural frequency we get resonance
YouTube - Ground Resonance - Side View
YouTube - breaking a wine glass using resonance
Let’s try some more questions!