
The problem asks to find the value of \( x \) given the time period of a simple pendulum of a specific length located at a height equal to the Earth's radius (\( R \)) above the Earth's surface.
The solution involves two key concepts from physics:
1. Time Period of a Simple Pendulum: The time period \( T \) of a simple pendulum is given by the formula:
\[ T = 2\pi\sqrt{\frac{L}{g_{\text{eff}}}} \]
where \( L \) is the length of the pendulum and \( g_{\text{eff}} \) is the effective acceleration due to gravity at the pendulum's location.
2. Variation of Gravity with Altitude: The acceleration due to gravity \( g' \) at a height \( h \) above the Earth's surface is related to the acceleration due to gravity on the surface (\( g \)) by:
\[ g' = g \left( \frac{R}{R+h} \right)^2 \]
where \( R \) is the radius of the Earth.
Step 1: Identify the given values.
Length of the pendulum, \( L = 4 \, \text{m} \).
Height above the Earth's surface, \( h = R \).
Time period of the pendulum, \( T = 2\pi \sqrt{\frac{8}{x}} \, \text{seconds} \).
Step 2: Calculate the acceleration due to gravity (\( g' \)) at the height \( h = R \).
Using the formula for variation of gravity with altitude:
\[ g' = g \left( \frac{R}{R+h} \right)^2 \]
Substitute \( h = R \):
\[ g' = g \left( \frac{R}{R+R} \right)^2 = g \left( \frac{R}{2R} \right)^2 = g \left( \frac{1}{2} \right)^2 \] \[ g' = \frac{g}{4} \]
Here, \( g \) is the acceleration due to gravity at the Earth's surface, which is approximately \( 9.8 \, \text{m/s}^2 \).
Step 3: Determine the time period of the pendulum at this height using its formula.
The time period \( T \) is given by:
\[ T = 2\pi\sqrt{\frac{L}{g'}} \]
Substitute the values \( L = 4 \, \text{m} \) and \( g' = g/4 \):
\[ T = 2\pi\sqrt{\frac{4}{g/4}} = 2\pi\sqrt{\frac{16}{g}} \]
Step 4: Equate the calculated time period with the given expression for the time period.
We are given \( T = 2\pi \sqrt{\frac{8}{x}} \). Equating this with our derived expression:
\[ 2\pi \sqrt{\frac{8}{x}} = 2\pi \sqrt{\frac{16}{g}} \]
Step 5: Solve the equation for \( x \).
Cancel \( 2\pi \) from both sides and square the equation:
\[ \left(\sqrt{\frac{8}{x}}\right)^2 = \left(\sqrt{\frac{16}{g}}\right)^2 \] \[ \frac{8}{x} = \frac{16}{g} \]
Now, solve for \( x \):
\[ 8g = 16x \] \[ x = \frac{8g}{16} = \frac{g}{2} \]
Substitute the standard value of \( g \approx 9.8 \, \text{m/s}^2 \) to find the numerical value of \( x \).
\[ x = \frac{9.8}{2} \] \[ x = 4.9 \]
Thus, the value of x is 5 (Nearest Integer)
A bullet of mass \(10^{-2}\) kg and velocity \(200\) m/s gets embedded inside the bob of mass \(1\) kg of a simple pendulum. The maximum height that the system rises by is_____ cm.
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

We can note there involves a continuous interchange of potential and kinetic energy in a simple harmonic motion. The system that performs simple harmonic motion is called the harmonic oscillator.
Case 1: When the potential energy is zero, and the kinetic energy is a maximum at the equilibrium point where maximum displacement takes place.
Case 2: When the potential energy is maximum, and the kinetic energy is zero, at a maximum displacement point from the equilibrium point.
Case 3: The motion of the oscillating body has different values of potential and kinetic energy at other points.