<40 kPa), and both the origami fluidic network and the origami strain-limiting layer unfold simultaneously. Therefore, the deployment ratio (\(\lambda=\frac{\left(L-L_0\right)}{L_0}\), where \(L\) is the effective layer length and \(L_0\) is its initial value), in response to applied fluidic pressure, rapidly increases compared to the bending angle (