Let the mass of the balloon be \( m = 60 \, {g} = 0.06 \, {kg} \).
When the balloon is moving upward with an acceleration of \( 4 \, {m/s}^2 \), the net force on the balloon is given by Newton’s second law: \[ F_{{net}} = m a \] where: - \( m = 0.06 \, {kg} \) is the mass of the balloon - \( a = 4 \, {m/s}^2 \) is the upward acceleration.
The upward force is: \[ F_{{up}} = m(g + a) = 0.06 \times (10 + 4) = 0.06 \times 14 = 0.84 \, {N} \] Now, to make the balloon move downward with the same acceleration, we need to add a mass to it, and the net force should be in the downward direction. For the downward motion, the net force is: \[ F_{{net}} = (m + M) \times a \] where \( M \) is the additional mass to be added. The downward force needed to get the balloon to descend with the same acceleration is equal to the force required to accelerate the added mass: \[ (m + M)(g - a) = F_{{up}} \quad \Rightarrow \quad (0.06 + M)(10 - 4) = 0.84 \] \[ (0.06 + M)(6) = 0.84 \] \[ 0.06 + M = \frac{0.84}{6} = 0.14 \] \[ M = 0.14 - 0.06 = 0.08 \, {kg} = 80 \, {g} \] Thus, the mass to be added to the balloon to make it descend with the same acceleration is \( 80 \, {g} \). \[ \boxed{80 \, {g}} \]
Sliding contact of a potentiometer is in the middle of the potentiometer wire having resistance \( R_p = 1 \, \Omega \) as shown in the figure. An external resistance of \( R_e = 2 \, \Omega \) is connected via the sliding contact.
The current \( i \) is :
For the reaction:
\[ 2A + B \rightarrow 2C + D \]
The following kinetic data were obtained for three different experiments performed at the same temperature:
\[ \begin{array}{|c|c|c|c|} \hline \text{Experiment} & [A]_0 \, (\text{M}) & [B]_0 \, (\text{M}) & \text{Initial rate} \, (\text{M/s}) \\ \hline I & 0.10 & 0.10 & 0.10 \\ II & 0.20 & 0.10 & 0.40 \\ III & 0.20 & 0.20 & 0.40 \\ \hline \end{array} \]
The total order and order in [B] for the reaction are respectively: