To solve this problem, we need to analyze the forces acting on the balloon and understand the changes needed for it to ascend with an acceleration \(a\).
Step 1: Current Scenario (Descending with Acceleration \(a\))
- When the balloon descends with acceleration \(a\), the net force acting downward is \(mg - T\), where \(T\) is the buoyant force or upthrust acting on the balloon.
- According to Newton's second law, the net force is given by:
\( T - mg = -ma \) because the balloon is accelerating downward.
- Rearranging the equation, we get:
\( T = m(g - a) \).
Step 2: New Scenario (Ascending with Acceleration \(a\))
- To ascend with acceleration \(a\), the net upward force must be positive.
- Let \(m_f\) be the final mass after removing some mass from the balloon.
- The equation becomes:
\(T - m_f g = m_f a\).
- Substituting the expression for \(T\) from Step 1:
\(m(g - a) - m_f g = m_f a\).
- Simplifying, we get:
\( m(g - a) = m_f (g + a) \).
Step 3: Mass to be Removed
- Solving for \(m_f\), we have:
\( m_f = \frac{m(g - a)}{g + a} \).
- The mass removed \(\Delta m\) is:
\( \Delta m = m - m_f \).
- Substituting for \(m_f\):
\( \Delta m = m - \frac{m(g - a)}{g + a} \).
- Simplifying further:
\( \Delta m = m \left( 1 - \frac{g - a}{g + a} \right) \)
- \( \Delta m = m \left( \frac{(g + a) - (g - a)}{g + a} \right) \), simplifying gives:
- \( \Delta m = m \left( \frac{2a}{g + a} \right) \).
Therefore, the mass that should be removed for the balloon to start ascending with acceleration \(a\) is \( \frac{2ma}{g+a} \).
Hence, the correct answer is: \( \frac{2ma}{g+a} \).