A block of mass m is placed on a smooth inclined wedge ABC of inclination θ as shown in the figure. The wedge is given an acceleration 'a' towards the right. The relation between a and θ for the block to remain stationary on the wedge is

1
a = \(\frac{g}{\text{cosec}\theta}\)
2
a = \(\frac{g}{\sin \theta}\)
3
a = g tan θ
4
More than one of the above
5
None of the above

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