To determine the pendulum bob's speed at its lowest point, accounting for energy loss due to air resistance, we first establish the initial potential energy. When released from a horizontal position, the bob possesses potential energy calculated as:
\[ E_{\text{initial}} = m \cdot g \cdot h \]
where:
Consequently, the initial energy is:
\[ E_{\text{initial}} = m \cdot 10 \cdot 10 = 100m \, \text{J} \]
The problem states that 10% of this initial energy is dissipated. This means 90% is converted into kinetic energy at the lowest point. Therefore, the energy at the lowest point is:
\[ E_{\text{kinetic}} = 0.9 \times 100m = 90m \, \text{J} \]
The kinetic energy at the lowest point is also defined by:
\[ E_{\text{kinetic}} = \frac{1}{2} m v^2 \]
Equating the available kinetic energy with this formula yields:
\[ \frac{1}{2} m v^2 = 90m \]
Upon canceling the mass (\(m\)) from both sides:
\[ \frac{1}{2} v^2 = 90 \]
Multiplying both sides by 2 to solve for \(v^2\):
\[ v^2 = 180 \]
Taking the square root of both sides gives the speed:
\[ v = \sqrt{180} = \sqrt{36 \cdot 5} = 6\sqrt{5} \, \text{ms}^{-1} \]
The bob's speed upon reaching the lowest point is thus \(6\sqrt{5} \, \text{ms}^{-1}\).
\( 6\sqrt{5} \, \text{ms}^{-1} \)
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is : 