91Ó°ÊÓ

1. The angle of the pendulum is
2. At $t=0,\mathrm{θ}=0.040\text{radand}\frac{\text{d}\mathrm{θ}}{\text{dt}}=-0.200\text{rad}/\text{s}$, and$\frac{\text{d}\mathrm{θ}}{\text{dt}}=-0.200\text{rad}/\text{s}$
   

The oscillations of the simple pendulum can be defined by the equation of simple harmonic motion. The simple harmonic motion is the motion in which the acceleration of the oscillating object is directly proportional to the displacement. The force caused by the acceleration is called restoring force. This restoring force is always directed towards the mean position.

Compare the given equation with the equation of displacement of the particle in simple harmonic motion.

Formulae:

$$\begin{gathered} x\left(t\right)=x_m\cos \left(\mathrm{Ó\neg }t+\mathrm{θ}\right) \\ v\left(t\right)=\mathrm{Ó\neg }{x}_m\sin \left(\mathrm{Ó\neg }t+\mathrm{θ}\right) \end{gathered}$$

The phase constant : $\mathrm{Φ}$

The expression for the displacement of the particle in simple harmonic motion is

$x\left(t\right)=x_m\text{cos}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)$

Here, x (t) is the displacement, x_m is amplitude, $\mathrm{Ó\neg }$angular velocity, t is time, $\mathrm{Φ}$ is phase difference.

For angular displacement, replace x by $\mathrm{θ}$, then

$\mathrm{θ}\left(t\right)={\mathrm{θ}}_m\cos \left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)$ …(¾±)

The expression for velocity of the particle in simple harmonic motion is

$v\left(t\right)=-\mathrm{Ó\neg }{x}_m\sin \left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)$

For angular motion, replace x by $\mathrm{θ}$, then

$\frac{d\mathrm{θ}}{dt}=-\mathrm{Ó\neg }{\mathrm{θ}}_m\text{sin}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)$ …(¾±¾±)

Divide equation (ii) by equation (i)

$\begin{array}{rcl}\frac{\frac{d\mathrm{θ}}{dt}}{\mathrm{θ}}& =& \frac{-\mathrm{Ó\neg }{\mathrm{θ}}_m\text{sin}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)}{{\mathrm{θ}}_m\text{cos}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)}\\ & =& \frac{-\mathrm{Ó\neg }\text{sin}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)}{\text{cos}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)}\\ & =& -\mathrm{Ó\neg }\text{tan}\left(\mathrm{Ó\neg }\text{t}+\mathrm{Φ}\right)\\ {\left(\frac{\frac{\text{d}\mathrm{θ}}{\text{dt}}}{\mathrm{θ}}\right)}_{t=0}& =& -\mathrm{Ó\neg }\text{tan}\left(\mathrm{Ó\neg }t+\mathrm{Φ}\right)\\ & =& -\mathrm{Ó\neg }\text{tan}\left(\mathrm{Φ}\right)\\ \mathrm{Φ}& =& {\text{tan}}^{-1}\left[-\frac{{\left(\frac{(\text{d}\mathrm{θ}/\text{dt}}{\mathrm{θ}}\right)}_{t=0}}{\mathrm{Ó\neg }}\right]\sqrt{a^2+b^2}\\ & =& {\text{tan}}^{-1}\left[-\frac{{\left(\frac{-0.200\text{rad}/\text{s}}{0.040\text{rad}}\right)}_{t=0}}{4.44\text{rad}/\text{s}}\right]\\ & =& 0.845\text{rad}\end{array}$

Therefore, the phase constant is 0.845 rad .

For t =0, equation (i) becomes as

$$\begin{gathered} \mathrm{θ}\left(\text{t}\right)={\mathrm{θ}}_m\text{cos}\left(\mathrm{Φ}\right) \\ {\mathrm{θ}}_m=\frac{\mathrm{θ}\left(t\right)}{\text{cos}\left(\mathrm{Φ}\right)} \\ =\frac{0.040\text{rad}}{\text{cos}\left(0.845\right)} \\ =0.0602\text{rad} \end{gathered}$$

The maximum angle is 0.0602 rad