A mass attached to a spring executes simple harmonic motion in a horizontal plane with an amplitude of 1.07 m. At a point 0.4815 m away from the equilibrium, the mass has speed 3.87 m/s.

What is the period of oscillation of the
mass? Consider equations for x(t) and v(t)
and use sin2 +cos2 = 1 to calculate !.
Answer in units of s.

i'm a bit confused after using the v(t) and x(t) with the cos and sin.

x = 1.07 sin (2 pi t/T)

dx/dt = v = (2 pi/T)(1.07) cos (2 pi t/T)

3.87 = 2 pi (1.07/T) cos(2 pi (1.07/T))
also
.4815 = 1.07 sin (2 pi (1.07)/T))

so
.5759 T = cos(mess)
.45 = sin (mess)

square everything
add
solve for T

To find the period of oscillation of the mass, we can use the equations for x(t) (displacement as a function of time) and v(t) (velocity as a function of time).

Let's start with the equation for x(t) for simple harmonic motion:

x(t) = A * cos(ωt) ---> Equation 1

where x(t) is the displacement at time t, A is the amplitude, ω is the angular frequency, and cos(ωt) represents the oscillatory motion.

We are given that the mass has a displacement of 0.4815 m away from equilibrium, which means x(t) = 0.4815 m. Plugging this value into equation 1 gives us:

0.4815 = A * cos(ωt)

Next, let's look at the equation for v(t), which is the derivative of x(t):

v(t) = -A * ω * sin(ωt) ---> Equation 2

where v(t) is the velocity at time t, ω is the angular frequency, and sin(ωt) represents the direction of the velocity.

We are given that the mass has a velocity of 3.87 m/s at the point 0.4815 m away from equilibrium. So v(t) = 3.87 m/s, and x(t) = 0.4815 m, which means:

3.87 = -A * ω * sin(ωt)

Now, we can use the information provided in the question to solve for the period of oscillation. We are given that the amplitude (A) is 1.07 m, and the speed at the specified point is 3.87 m/s. Using the relationship between speed (v) and angular frequency (ω):

v = A * ω

we can solve for ω:

ω = v / A = 3.87 m/s / 1.07 m = 3.62 rad/s

We can substitute this value of ω into Equation 1 and Equation 2 to find cos(ωt) and sin(ωt):

0.4815 = 1.07 * cos(3.62t)
3.87 = -1.07 * 3.62 * sin(3.62t)

Using the trigonometric identity sin^2 + cos^2 = 1, we can solve for sin(3.62t):

sin^2(3.62t) + cos^2(3.62t) = 1
(sin(3.62t))^2 = 1 - (cos(3.62t))^2

Substituting the values we obtained earlier:

(sin(3.62t))^2 = 1 - (0.4815 / 1.07)^2

Simplifying further:

(sin(3.62t))^2 = 1 - 0.2016
(sin(3.62t))^2 = 0.7984

We can take the square root of both sides to find sin(3.62t):

sin(3.62t) = sqrt(0.7984)

Now, we can solve for the period (T) of the oscillation using the relationship between angular frequency (ω) and period (T):

T = 2π / ω = 2π / 3.62 rad/s

Calculating this value, we get:

T ≈ 1.733 s

So, the period of oscillation of the mass is approximately 1.733 seconds.