Patent ID: 8803822

Claim:
A time-reversal-based impact-localization and haptic-feedback method for touch panels, comprising steps: constructing a plate model of an elastic plate according a plate theory, wherein said plate model is constructed according to a plurality of material parameters of said elastic plate, including thickness, unit impulse density and bending stiffness, Young's modulus, and a Poisson ratio of said elastic plate; calculating an impulse response d i (t) of an arbitrary point i of said elastic plate in accordance with: d i ⁡ ( t ) = ∑ i = 1 L ⁢ ⁢ w il ⁡ ( x , y , t ) ⊗ r l ⁡ ( t ) , wherein {circle around (x)} is the linear time convolution, i is the number of the touchable points on the elastic plate, r i (t) is the force applied to the elastic plate, wherein l=1, 2, . . . , L, wherein L is the number of a sensor, and w il (x,y,t) is the transfersal displacement of said arbitrary point i described by said plate model d i (t); using a time-reversal approach to construct a mathematic model according to said impulse response; using at least one sensor at a corner of said elastic plate to receive a touch signal generated via applying an external force to a touched point of said elastic plate; and using a simulator to convert said touch signal into as thine-reversal signal according to said time-reversal approach and retransmit said time-reversal signal emitted by said at least one sensor to said touched point to simulate a waveform of backward-propagation vibration and position said touched point, wherein said feedback-induced vibration is simulated in accordance with w il ⁡ ( x , y , t ) = ∑ m = 1 ∞ ⁢ ⁢ ∑ n = 1 ∞ ⁢ ⁢ 4 Ω mn ⁢ abh ⁢ ⁢ ρ ⁢ sin ⁢ m ⁢ ⁢ π ⁢ ⁢ x i a ⁢ sin ⁢ n ⁢ ⁢ π ⁢ ⁢ y i b ⁢ sin ⁢ m ⁢ ⁢ π ⁢ ⁢ x l a ⁢ sin ⁢ n ⁢ ⁢ π ⁢ ⁢ y l b ⁢ sin ⁡ ( Ω mn ⁢ t ) . wherein ρ is the density of the elastic plate, w is the transversal displacement, h is the thickness of the elastic plate, (x 0 , y 0 ) is the touched point, and wherein D is the bending stiffness per unit length expressed by D = Eh 3 12 ⁢ ( 1 - υ 2 ) , wherein E and ν are the Young's modulus and Poisson ratio of the elastic plate, respectively, and wherein Ω mn = D ρ ⁢ ⁢ h [ ( m ⁢ ⁢ π a ) 2 + ( n ⁢ ⁢ π b ) 2 ] , wherein a and b are the length and width of the elastic plate, respectively.