To understand how acceleration due to gravity changes with depth and height relative to Earth's surface, we analyze two key scenarios.
1. Acceleration at Depth (gdepth):
The acceleration due to gravity at depth $d$ below Earth's surface is given by:
$ g_{\text{depth}} = g_{\text{surface}} \left( 1 - \frac{d}{R} \right) $
where:
- $g_{\text{surface}}$ = surface gravity (9.8 m/s²)
- $R$ = Earth's radius
- $d$ = depth below surface
This can alternatively be expressed as:
$ g_{\text{depth}} = g_{\text{surface}} \left( \frac{r}{R} \right) $
where $r = R - d$ is the distance from Earth's center.
2. Acceleration at Height (gheight):
For height $h$ above the surface:
$ g_{\text{height}} = g_{\text{surface}} \left( \frac{R^2}{(R + h)^2} \right) $
3. Key Observations:
a) At Earth's center ($d = R$):
$ g_{\text{depth}} = 0 $ (gravity cancels out)
b) At surface ($d = 0$):
$ g_{\text{depth}} = g_{\text{surface}} $ (maximum value)
c) Above surface ($h > 0$):
Gravity decreases with height as the denominator $(R + h)^2$ grows.
4. Conclusion:
Gravity increases linearly from center to surface, then decreases inversely with square of distance above surface. The governing equations are:
For depth: $ g_{\text{depth}} = g_{\text{surface}} \left( 1 - \frac{d}{R} \right) $
For height: $ g_{\text{height}} = g_{\text{surface}} \left( \frac{R^2}{(R + h)^2} \right) $
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: