10A.2 SHM Mathematics Flashcards
the motion of the oscillation in SHM is a
projection of motion in a circle so all the circle equations work within SHM
what is the displacement of an object in SHM
x = r cos (wt) derivation page 155,
all simple harmonic oscillators can be described by
a sin, or cosine function which gives their displacement, velocity and acceleration over time
the displacement of a pendulum is = to
x = A cos(wt) r of circle is replaced with the amp as at t = o x= A
the restoring force over time is given as
f = - k A cos(wt) since x = A cos(wt)
using the restoring force and N2L of motion the a =
a = - k/m A cos(wt) derivation page 155
from a = - k/m A cos(wt) we can tell
that acceleration and displacement in SHM have the same form, just acceleration acts in the opposite direction, so when x is at zero so is a and when x is at max so is a
how do we find the velocity from x = A cos(wt)
by differentiating x to get dx/dt which is the gradient of the graph and the gradient of a x/t graph is V so v = -Awsin(wt)
how do we find acceleration from x = A cos(wt)
by differentiating x to get dx/dt which is the gradient of the graph, and the gradient of a x/t graph is V so v = -Awsin(wt), the differentiating a second time to get dv/dt or d^2x/dt^2 which dv/dt = to the gradient of a v/t graph which is equal to acceleration so a = -Aw^2cos(wt) or -w^2x since x = A cos(wt)
if we know that mass of a oscillating object, and we know the angular velocity of an object we can find the restoring force constant k via
k = w^2 m (derivation page 156)
what is the max values of v and a in SHM given that cos and sin max values are 1
v max = - Aw(max)
a max = -Aw^2