Heat generating resistor, recording head using such resistor and drive method therefor

Claim 2

A planar heat generating resistor which has a heat generating resistor layer formed on or above a support member and a pair of opposing electrodes formed on the heat generating resistor layer a width of the heat generating resistor layer at the electrode area being larger than a width of the electrodes and a voltage being applied across the electrodes, wherein a ratio of a maximum value of a gradient of φ, √(∂φ/∂x) 2 +(∂φ/∂y) 2 to a value of √(∂φ/∂x) 2 +(∂φ/∂y) 2 at a center of the resistor is no larger than 1.4 when a Laplace equation ∂ 2 φ/∂x 2 +∂ 2 φ/∂y 2 =0 is solved for the heat generating resistor when an orthogonal coordinate system X-Y is defined on the resistor surface, a potential at a point (x,y) on the resistor surface is represented by φ(x,y), a boundary value is imparted to an area of a circumferential boundary of the resistor which contacts to one of the electrodes, a different boundary value is imparted to an area which contacts to the other electrode, and a boundary condition in which a differential coefficient of φ to a normal direction of the circumferential boundary is zero is imparted to an area which does not contact to any of the electrodes.

Claim 3

A liquid jet recording head comprising an orifice for discharging liquid, a liquid flow path communicating with the orifice, a heat generating resistor arranged in the liquid flow path for generating thermal energy to discharge the liquid, the heat generating resistor including a heat generating resistor layer formed on or above a support member and a pair of opposing electrodes formed on the heat generating resistor layer, a width of the heat generating resistor layer at an electrode area being larger than a width of the electrodes, a voltage being applied across the electrodes, the heat generating resistor having a ratio of no larger than 1.4 of a maximum value of a gradient φ, √(∂φ/∂x) 2 +(∂φ/∂y) 2 to a value of √(∂φ/∂x) 2 +(∂φ/∂y) 2 at a center of the resistor when a Laplace equation ∂ 2 φ/∂x 2 +∂ 2 φ/∂y 2 =0 is solved for the heat generating resistor area when an orthogonal coordinate system X-Y is defined on a surface of the resistor, a potential at a point (x,y) on the resistor surface is represented by φ(x,y), a boundary value is imparted to an area of a circumferential boundary of the resistor which contacts to one of the electrodes, a different boundary value is imparted to an area which contacts to the other electrode, and a boundary condition in which a differential coefficient of φ to a normal direction of the circumferential boundary is imparted to an area which does not contact to any of the electrode.

Claim 4

A liquid jet recording head comprising an orifice for discharging liquid, a liquid flow path communicating with the orifice, a heat generating resistor arranged in the liquid flow path for generating thermal energy to discharge the liquid, the heat generating resistor including a heat generating resistor layer formed on or above a support member and a pair of opposing electrodes formed on the heat generating resistor layer, a width of the heat generating resistor layer at an electrode area being larger than a width of the electrodes, a voltage being applied across the electrodes, the heat generating resistor having a ratio of no larger than 1.4 of a maximum value of a gradient φ, √(∂φ/∂x) 2 +(∂φ/∂y) 2 to a value of √(∂φ/∂x) 2 +(∂φ/∂y) 2 at a center of the resistor when a Laplace equation ∂ 2 φ/∂x 2 +∂ 2 φ/∂y 2 =0 is solved for the heat generating resistor area when an orthogonal coordinate system X-Y is defined on a surface of the resistor, a potential at a point (x,y) on the resistor surface is represented by φ(x,y), a boundary value is imparted to an area of a circumferential boundary of the resistor which contacts to one of the electrodes, a different boundary value is imparted to an area which contacts to the other electrode, and a boundary condition in which a differential coefficient of φ to a normal direction of the circumferential boundary is imparted to an area which does not contact to any of the electrode.

Claim 5

A recording head having a heat generating resistor according to claim 1.

Claim 6

A planar heat generating resistor according to claim 1, wherein said resistor has a lower layer between said support member and said heat generating layer.

Claim 7

A planar heat generating resistor according to claim 1, wherein said resistor has an upper layer on said heat generating resistor layer.

Claim 8

A liquid jet recording head having a heat acting area communicating with an orifice for discharging liquid for forming bubbles in the liquid by applying thermal energy to the liquid, and a heat generating resistor for generating the thermal energy, the heat generating resistor including a heat generating resistor layer formed on a lower layer formed on or above a support member and a pair of opposing electrodes formed on the heat generating resistor layer, a width of the heat generating resistor at an electrode area being larger than a width of the electrodes, a voltage being applied across the electrodes, an upper layer being formed on the heat generating resistor, the heat generating resistor having a ratio of no larger than 1.8 of a maximum value of a gradient of φ, √(∂φ/∂x) 2 +(∂φ/∂y) 2 to a value of √(∂φ/∂x) 2 +(∂φ/∂y) 2 at a center of the resistor when a Laplace equation ∂ 2 φ/∂x 2 +∂ 2 φ/∂y 2 =0 is solved for the area of the heat generating resistor when an orthogonal coordinate system X-y is defined on a surface of the heat generating resistor, φ(x,y) is defined as a potential at a point (x,y) on the surface of the resistor, a boundary value is imparted to an area of a circumferential boundary of the resistor which contacts to one of the electrodes, a different boundary value is imparted to an area which contacts to the other electrode, and a boundary condition in which a differential coefficient of φ to a normal direction of the circumferential boundary is zero is imparted to an area which does not contact to any of the electrodes, and the heat generating resistor meeting the following condition ##EQU23## where k(x) is a thermal conductivity of a material at a position x measured in the direction of the lower layer from the boundary of the layer and the support member to the heat acting area, c(x) is a specific heat, ρ(x) is a density, L is a total thickness from the boundary of the lower layer and the support member of the heat generating resistor and τ B is a time from start of application of the heat energy to extinguishment of the bubbles.

Claim 9

A liquid jet recording head having a heat acting area communicating with an orifice for discharging liquid for forming bubbles in the liquid by applying thermal energy to the liquid, and a heat generating resistor for generating the thermal energy, the heat generating resistor including a heat generating resistor layer formed on a lower layer formed on or above a support member and a pair of opposing electrodes formed on the heat generating resistor layer, a width of the heat generating resistor at an electrode area being larger than a width of the electrodes, a voltage being applied across the electrodes, an upper layer being formed on the heat generating resistor, the heat generating resistor having a ratio of no larger than 1.8 of a maximum value of a gradient of φ, √(∂φ/∂x) 2 +(∂φ/∂y) 2 to a value of √(∂φ/∂x) 2 +(∂φ/∂y) 2 at a center of the resistor when a Laplace equation ∂ 2 φ/∂x 2 +∂ 2 φ/∂y 2 =0 is solved for the area of the heat generating resistor when an orthogonal coordinate system X-y is defined on a surface of the heat generating resistor, φ(x,y) is defined as a potential at a point (x,y) on the surface of the resistor, a boundary value is imparted to an area of a circumferential boundary of the resistor which contacts to one of the electrodes, a different boundary value is imparted to an area which contacts to the other electrode, and a boundary condition in which a differential coefficient of φ to a normal direction of the circumferential boundary is zero is imparted to an area which does not contact to any of the electrodes, and the heat generating resistor meeting the following condition ##EQU23## where k(x) is a thermal conductivity of a material at a position x measured in the direction of the lower layer from the boundary of the layer and the support member to the heat acting area, c(x) is a specific heat, ρ(x) is a density, L is a total thickness from the boundary of the lower layer and the support member of the heat generating resistor and τ B is a time from start of application of the heat energy to extinguishment of the bubbles.

Claim 12

A method according to claim 7 wherein, said voltage Vop satisfies the relationship Vop≦1.3 Vth wherein Vth is a minimum value of the applied voltage by which said bubbles for discharging the liquid are generated is generated.

Claim 13

A method according to claim 7, wherein said heat generating resistor has a lower layer between said support member and said heat generating resistor layer.

Claim 14

A method according to claim 8, wherein said heat generating resistor has an upper layer on said heat generating resistor layer.