Abstract:
An electric energy auxiliary device of transdermal drug delivery patch is provided which includes an upper electrode, a lower electrode, and a drug storage area between two electrodes, generating a kinetic energy in the pharmaceutical compound in the drug storage area toward the skin by a electric field between two electrodes. For the pharmaceutical compound with the same polarity, the pharmaceutical compound is pushed by the electric energy interacted with polar the pharmaceutical compound so as to deliver the drug the human body. The lower electrode generates an ion channel with electroporation on the surface of skin. By using the change of electric field on the surface of skin, a temporary ion channel is generated in the cells where the pharmaceutical compound enters the systemic circulation of human body via skin. This temporary ion channel allows large compound to pass into the skin of human body.

Description:
BACKGROUND OF THE INVENTION  
       [0001]     1. Field of the Invention  
         [0002]     The invention relates to a drug delivery technology, and, more particularly, to an electric energy auxiliary device of transdermal drug delivery patch which can be applied to the treatment for systemic disease or the field of transporting the pharmaceutical compounds or ions by the transdermal way.  
         [0003]     2. Description of the Prior Art  
         [0004]     Recently, transdermal route has vied with oral and injection treatments as the most successful innovative research region in drug delivery. It will be a future choice for systemic delivery of protein and peptide with large compound, which usually can only be delivered by parenteral therapy. In worldwide transdermal patch market, there exist only ten drugs, such as scopolamine, nitroglycerine, clonidine, etc. In these drugs, their delivery is generally passive, which has a low skin-penetration capability. Thus, electrically assisted methods are required to improve drug delivery efficiency of the passive diffusion.  
         [0005]     In general, drug delivery involves either chemical or physical processing, or both, including the oral treatment, intravenous, intramuscular, subcutaneous, transdermal patch, iontophoresis, electroporation. With chemical processing, drug may be remained in skin surface or interacted with human body, resulting in hurting organism. Compared with chemical processing, the physical one is more safe for drug delivery, and it is usually in a transdermal way. Transdermal drug delivery (TDD) is divided into two categories: active and passive ones. To attain safe and comfortable drug delivery, active methods are usually used to deliver drugs with electrical assistance. In conventional electrical assistance, processes of iontophoresis and electroporation are used for TDD. The iontophoretic delivery system is shown in  FIG. 1 , which comprises a set of positive electrode  10  and negative electrode  12  positioned on the surface of skin  14 . By using the attraction and the pushing between the electric field and the pharmaceutical compounds  16 , the pharmaceutical compounds  16  are delivered into the blood vessel  20  of the deeper stratum  18  (systemic circulation of human body). Another iontophoretic delivery system comprises their electrodes having two sets of metallic film for applying pulsed voltages to the patch to increase drug-penetration capability. Skin electroporation creates transient aqueous pore in the lipid bilayers by application of short electrical pulses processes of electroporation can be illustrated by FIGS.  2 ( a ) to  2 ( e ). The normal cell membrane  70  is shown in  FIG. 2 ( a ). The cell membrane  70  is excited by short electrical pulses resulting in irregular compound structure shown in  FIG. 2 ( b ). If the water-solube compound concentration outside the cell membrane  70  is high, the outer of adipose stratum will be destroyed causing the cell membrane  70  notched, shown in  FIG. 2 ( c ). The cell membrane  70  with a temporary hydrophobic pore  84  is formed shown in  FIG. 2 ( d ). The cell membrane  70  with a hydrophilic pore  86  is formed after membrane restructuring, shown in  FIG. 2 ( e ). These pores provide pathways for penetration, from which the charged compounds and ions travel straightforwardly through the cell membrane  70 . After the voltage of electroporation is removed, the cell membrane  70  is restored to be a normal cell membrane of  FIG. 2 ( a ).  
         [0006]     Electrically-activates devices have been described in U.S. Pat. No. 6,377,848 shown in  FIG. 3 , comprising a control circuitry, a set of electrodes and the drug. The devices transport drug into the human baby by an iontophoretic drug delivery. The devices include a power source  28 , a patch  30  and the electronic interconnectors  32  of the power source  28 . The patch  30  includes the positive electrode  34  and the negative electrode  36 . The patch  30  includes the positive electrode  34  and the negative electrode  36  positioned respectively in the reservoirs  38  and  40 . The patch  30  is attached to the surface of the skin  42 . The power source  28  provides the electric energy to the electrodes  34  and  36  by the electronic interconnectors  32 . The polarity of the electrode  36  is negative, and the polarity of the electrode  34  is positive. Since the drug in the reservoirs  38  and  40  are the ionized negatively drug, the negative polarity of the electrode  36  is repulsed with the negative polarity of the ionized drug due to the same charge, thereby generating a force across the skin  42 . The drug is delivered into the deeper tissues of the skin  42  by this force. When the pharmaceutical compound is delivered into the deeper tissues of the skin  42 , the negative polarity of the ionized drug is neutralized due to electrolysis stratum in the most bottom of stratum corneum. The pharmaceutical compound across stratum corneum of the skin is unable to penetrate more deeper, only maintaining in the corneum. To solve this problem, an iontophoretic delivery system is provided. The positive ions in the electrolysis stratum is interacted with the negative electrode, thereby attracting the positive ions from the electrolysis stratum, so as the negatively ionized drug can penetrate through skin and enter the blood vessel.  
         [0007]     However, a problem may sexist because it takes some time to reach the treatment concentration in the blood vessel when using the patch with an iontophoretic delivery method. In additional, this two-electrodes structure may cause the polarization of electrode. When the overpotential is generated, it is uncomfortable for the patient. As these problems previously, the poisonous material will be generated to cause the injury for the patient.  
       SUMMARY OF THE INVENTION  
       [0008]     An object of the present invention is to provide an electric energy auxiliary device of transdermal drug delivery patch with a multi-electrode structure having drug delivery efficiency of iontophoresis, electroporation, and natural diffusion.  
         [0009]     Another object of the present invention is to provide an electric energy auxiliary device of transdermal drug delivery patch that provides a strongly thrust by using two-electrodes structure to deliver the pharmaceutical compounds into the human body readily.  
         [0010]     Another object of the present invention is to provide an electric energy auxiliary device of transdermal drug delivery patch, thereby generating the rotational electric field by the lower electrode, preventing the skin from the single direction of electric field so as to reduce the polarization of electrodes.  
         [0011]     Another object of the present invention is to provide an electric energy auxiliary device of transdermal drug delivery patch, not being subjected to the size and hydrophile of pharmaceutical compound so as to improve effectiveness of drug delivery.  
         [0012]     Another object of the present invention is to provide an electric energy auxiliary device of transdermal drug delivery patch, which is used in drug delivery system with the polar and neutral pharmaceutical compounds.  
         [0013]     On one aspect of the present invention, an electric energy auxiliary device of transdermal drug delivery patch is provided which includes an upper electrode, a lower electrode, and a drug storage area between two electrodes, generating a kinetic energy in the pharmaceutical compounds in the drug storage area toward the skin by an electric field between two electrodes. For the pharmaceutical compounds with the same polarity, the pharmaceutical compounds are pushed by the electric energy interacted with the polar pharmaceutical compound so as to deliver the drug into the human body. The lower electrode generates an ion channel with electroporation on the surface of skin. By using the change of electric field on the surface of skin, a temporary ion channel is generated in the cells where the pharmaceutical compounds enter the systemic circulation of human body via skin. This temporary ion channel allows the large compound to pass into the skin of human body.  
         [0014]     In another aspect of the present invention, a thin film is provided to control the release rate of the pharmaceutical compounds. The thin film is attachable to the adhesion layer of skin, and covered over the backing of the outer surface of the upper electrode. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0015]     These and other objects, features and advantages of the present invention can best be understood by reference to the detailed description of the preferred embodiments set forth below taken with the drawings, in which:  
         [0016]      FIG. 1  is a schematic view of the iontophoretic drug delivery system in accordance with the prior art;  
         [0017]     FIGS.  2 ( a ) through  2 ( e ) are schematic views of a cell membrane excited by short electrical pulses;  
         [0018]      FIG. 3  shows a block diagram of an iontophoretic drug delivery device in accordance with the U.S. Pat. No. 6,377,848;  
         [0019]      FIG. 4  shows a block diagram of electric energy auxiliary device of transdermal drug delivery patch in accordance with the present invention;  
         [0020]      FIG. 5  is a moving diagram illustrating the charged particles in uniform electric field in accordance with the present invention;  
         [0021]      FIG. 6  is a motion diagram illustrating the charged particles in uniform magnetic field in accordance with the present invention;  
         [0022]      FIG. 7  is a diagram illustrating the positive particles forced by an electric field in accordance with the present invention;  
         [0023]      FIG. 8 a  graph of the magnetic flux {right arrow over (B)} versus the electric field in the time-varied electric field in accordance with the present invention;  
         [0024]      FIG. 9 a  vector diagram of the positive particles versus the magnetic field in the time-varied electric field in accordance with the present invention;  
         [0025]      FIG. 10 a  vector diagram of the force {right arrow over (F)} c  combined the force of electric field {right arrow over (F)} e  with the force of magnetic field {right arrow over (F)} m  in accordance with the present invention;  
         [0026]      FIG. 11 a  vector diagram of two active electrodes versus the force of an ion in accordance with the present invention;  
         [0027]      FIG. 12  shows a block diagram of two active electrodes in accordance with the present invention;  
         [0028]      FIG. 13  shows a block diagram illustrating a single set of upper electrode and two sets of lower electrodes in accordance with the present invention;  
         [0029]      FIG. 14  is a drive timing diagram illustrating the positive electrode drug transport in accordance with the present invention;  
         [0030]      FIG. 15  is a relative position diagram of electric field component having xy plane formed by electric field versus a pharmaceutical compound in accordance with the present invention;  
         [0031]      FIG. 16  is a relative position diagram of electric field component having xz plane formed by electric field versus a pharmaceutical compound in accordance with the present invention;  
         [0032]      FIG. 17  is a relative position diagram of electric field component having xy, yz, and zx plane formed by electric field versus a pharmaceutical compound in accordance with the present invention;  
         [0033]      FIG. 18  is a vector diagram of the resulting force {right arrow over (F)} c1  interacting with {right arrow over (F)} e1  and {right arrow over (F)} m1  in accordance with the present invention;  
         [0034]      FIG. 19  is a vector diagram of the resulting force {right arrow over (F)} c2  interacting with {right arrow over (F)} e2  and {right arrow over (F)} m2  in accordance with the present invention;  
         [0035]      FIG. 20  is a vector diagram of the resulting force {right arrow over (F)} c3  interacting with {right arrow over (F)} E  and {right arrow over (F)} mx , {right arrow over (F)} my  and {right arrow over (F)} mz  in accordance with the present invention;  
         [0036]      FIG. 21  shows a block diagram illustrating a single set of upper electrode and three sets of lower electrodes in accordance with the present invention;  
         [0037]      FIG. 22  shows a block diagram illustrating a single set of upper electrode and four sets of lower electrodes in accordance with the present invention;  
         [0038]      FIG. 23  is a diagram of the driving way illustrating three sets of lower electrodes in accordance with the present invention;  
         [0039]      FIG. 24  is a diagram of the driving way illustrating four sets of lower electrodes in accordance with the present invention;  
         [0040]      FIG. 25  is a drive timing diagram illustrating the negative electrode drug transport in accordance with the present invention;  
         [0041]      FIG. 26  is a relative position diagram of electric field component having xy plane formed by electric field versus a pharmaceutical compound in accordance with the present invention;  
         [0042]      FIG. 27  is a relative position diagram of electric field component having xz plane formed by electric field versus a pharmaceutical compound in accordance with the present invention;  
         [0043]      FIG. 28  is a relative position diagram of electric field component having xy, yz, and zx plane formed by electric field versus a pharmaceutical compound in accordance with the present invention;  
         [0044]      FIG. 29 a  vector diagram of the resulting force {right arrow over (F)} c4  interacting with {right arrow over (F)} e4  and {right arrow over (F)} m4  in accordance with the present invention;  
         [0045]      FIG. 30 a  vector diagram of the resulting force {right arrow over (F)} c5  interacting with {right arrow over (F)} e5  and {right arrow over (F)} m5  in accordance with the present invention; and  
         [0046]      FIG. 31  is a vector diagram of the resulting force {right arrow over (F)} c6  interacting with {right arrow over (F)} E  and {right arrow over (F)} mx , {right arrow over (F)} my  and {right arrow over (F)} mz  in accordance with the present invention. 
     
    
     DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0047]     The present invention provides an electric energy auxiliary device of transdermal drug delivery patch with a multi-electrode structure, which improves the active and passive Transdermal drug delivery (TDD) of the prior art. When using the patch of the present invention, the present invention provides a strongly thrust by using two-electrode structure to deliver the pharmaceutical compound into the human body readily, thereby preventing the polarization of electrodes from the treatment, so as to reduce uncomfortable feeling for the patient.  
         [0048]     An electric energy auxiliary device  50  of transdermal drug delivery patch attached to the skin  52  of human body in accordance with the present invention, as shown in  FIG. 4 , includes a two-electrode structure, the upper electrode  54  and the lower electrode  56 , which are respectively formed of any shape of electrode array, The time-varied voltage is applied on the upper electrode  54  and the lower electrode  56 . A drug storage area  58  is placed between the upper electrode  54  and the lower electrode  56 . A thin film  60  is positioned between the drug storage area  58  and the lower electrode  56  to control the release rate of pharmaceutical compound in the drug storage area  58 . A layer of a backing  62  is covered over the outer surface of the upper electrode  54 . An adhesion layer  64  is positioned between the lower electrode  56  and the thin film  60  to cover the top surface of the lower electrode  56  so as to attach to the skin of human body. In the electric energy auxiliary device  50 , by using the rotational electric field by the upper electrode  54  and the lower electrode  56 , a kinetic energy is generated in pharmaceutical compound in the drug storage area  58  toward the skin  52 . The lower electrode  56  generates a temporary ion channel with electroporation on the surface of skin  52 , allowing pharmaceutical compound across through the skin  52  easily, so as to deliver the drug into the human body rapidly.  
         [0049]     The present invention has been already disclosed. The detailed principle of the present invention is described herein. The present invention can be presented to a user, and the user can visually understand the present invention.  
         [0050]     In nature, the electromagnetic force, the gravitational force, the strong force, and the weak force are called the fundamental forces. The electromagnetic force and daily life are closely related. Also, the electromagnetic force is the power source of Transdermal Drug Deliver. The action force relationship between the electromagnetic force and the matter relates to the amount of charge carried by the matter. When the charged particle is positioned in the uniform electromagnetic field, the force is represented by the following equation (1), 
 
 {right arrow over (F)}=q ( {right arrow over (E)}+{right arrow over (V)}×{right arrow over (B)} )   (1) 
 
         [0051]     where {right arrow over (F)} is the force which the charged particle is subjected to the uniform electromagnetic field, which combines the electric filed force with the magnetic field force, q is the charge amount of charged particle, {right arrow over (E)} is the electric field intensity, {right arrow over (V)} is the moving velocity after the charged particle is subjected to the electric filed, and {right arrow over (B)} is magnetic flux density. The forces between the electric filed, magnetic field, and the matter are described as the followings:  
         [0052]     (a) The force which the charged particle is subjected to the electric filed  
         [0053]     The movement which the charged particle is subjected to the uniform electric field is shown in  FIG. 5 . {right arrow over (F)} e  is the force which the electric field is applied on the charged particle. X, Y and z are the directions of right angle coordinate. When the charged particle is positioned in the uniform electric field, the positive charged particle is moving toward the negative electrode (lower electrode)  56  due to the electric field, and the negative charged particle is moving toward the positive electrode (upper electrode)  54 . The charged particle in the uniform electric field is subjected to a force. The force is determined by the following equation (2). 
 
{right arrow over (F)} e =q{right arrow over (E)}  (2) 
 
         [0054]     Where {right arrow over (F)} e  is the force which the charged electric field is applied on the charged particle, and {right arrow over (E)} is the electric field intensity.  
         [0055]     (b) The force which the charged particle is subjected to the magnetic field  
         [0056]     The movement which the charged particle is subjected to the uniform magnetic field is shown in  FIG. 6 . {right arrow over (F)} e  is the force which the electric field is applied on the charged particle. X, Y and z are the directions of right angle coordinate. When the charged particle is positioned in the uniform magnetic field and the charged particle is subjected to the magnetic effect, the force, which is perpendicular to the magnetic field and the moving direction, is produced. The force is determined by the following equation (3). 
 
 {right arrow over (F)}   m   =q{right arrow over (V)}×{right arrow over (B)}   (3) 
 
 where {right arrow over (F)} m  is the force which the magnetic field is applied on the charged particle, q is the charge amount of charged particle, {right arrow over (V)} is the moving velocity of the charged particle, and {right arrow over (B)} is magnetic flux density. According to the aforementioned equation, it found that the forces of electric field and the force of magnetic field are produced in sequence when a charged particle is positioned in the uniform electromagnetic field. The total force, which the charged particle is subjected to the electromagnetic field, is obtained by combining with these two forces. The total force is determined by the following equation (4). 
 
 {right arrow over (F)}={right arrow over (F)}   e   +{right arrow over (F)}   m   =q(   {right arrow over (E)}+{right arrow over (V)}×{right arrow over (B)})    (4) 
 
         [0057]     If a positive particle is positioned in the electric field changing as the time, the relationship between the time-varied electric field and the magnetic field is determined by the Maxwell equation, as the following equation (5),  
               ∇     ×     E   ⇀         =     -       ∂     B   ⇀         ∂   t                 (   5   )             
 
 where {right arrow over (E)} is the electric field changing as the time, and {right arrow over (B)} is magnetic flux density. According to the equation (5), a time-varied electric field in the space can induce the magnetic field changed by the time, and the resulting force is obtained by combining the force of the electric field with the electromagnetic field. 
 
         [0058]     According to the Maxwell equation, if a charged particle is positioned in the time-varied electric field, the charged particle is subjected to the electric field first, and the force {right arrow over (F)} e  is produced, as shown in  FIG. 7 . The force of electric field is profiled on the xy plane. The vector {right arrow over (E)} u  of electric field is represented by the equation (6). 
 
 {right arrow over (E)}   u   ={right arrow over (E)}   x ( x,y,t ) {right arrow over (i)}   x   +E   y ( x,y,t ){right arrow over (i)} y    (6) 
 
 where {right arrow over (E)} u  is the vector of electric field, Ey is the vector component of axis y in the electric field {right arrow over (E)} u , and Ex is the vector component of axis x in the electric field {right arrow over (E)} u . Since {right arrow over (E)} u  is the time-varied electric field, the equation (6) is conducted into the equation (5). The math relationship equation between the time-varied electric field and the time-varied magnetic field is represented by the equation (7).  
                 (         ∂     E   y         ∂   x       -       ∂     E   x         ∂   y         )     ⁢           ⁢       i   ⇀     z       =       -     ⅆ     ⅆ   t         ⁢     B   ⇀     ⁢       i   ⇀     z               (   7   )             
 
 where ∂E y /∂x is the partial derivative of variable of x in E y  function, ∂E x /∂y is the partial derivative of variable of y in E x  function, and {right arrow over (i)} z  is the vector of unit direction of axis z. The induced magnetic flux {right arrow over (B)} and the vector of electric field are represented in  FIG. 8 . 
 
         [0059]     According to the equation (7), when the time-varied electric field generates an alternating magnetic filed {right arrow over (B)} (−{right arrow over (i)} z) in the space, there is a force {right arrow over (F)} m  applied on the charged particle. The vector relationship between the force {right arrow over (F)} m  and the magnetic flux is shown in  FIG. 9 . {right arrow over (v)} ({right arrow over (i)} x )is the moving velocity of displacement produced by the charged particle in the electric field. The moving charged particle is subjected to the magnetic force {right arrow over (F)} m  in the magnetic field. According to the equation (3), {right arrow over (F)} m  of vector of direction is the direction of negative axis y. According to the aforementioned analysis, it found that a charged particle positioned in the alternating electric field is subjected to the force of electric field and the induced force of magnetic field simultaneously. The magnitude and direction of resulting force are obtained by the equation (1). Their vector relationship is shown in  FIG. 10 .  
         [0060]     To sum up, the upper electrode  54  and the lower electrode  56  of the present invention are respectively positioned on the xy planes, and the pharmaceutical compound  16  with the polarity is positioned between two electrodes  54  and  56 . The time-varied voltage is applied on the upper electrode  54  and the lower electrode  56 . The space, which is the drug positioned in, exerts the force of electric field and the force of magnetic field simultaneously. The resulting vector of two forces is profiled on the xy plane. Therefore, the patch is attachable to the skin of human  52 . The relative position of skin of human  52  on coordinate axis is on the xy plane, and is adjacent with the lower electrode  56  in order to move the pharmaceutical compound toward the skin  52  by the resulting electromagnetic force. This resulting force makes the pharmaceutical compound moving toward the surface of skin, shown in  FIG. 11 . In the present invention, the structure of lower electrode is the combination of multi-electrode. This set of multi-electrode is contacted with the skin directly. When an external voltage is applied on this set of electrodes, a temporary ion channel is produced in the obstacle cell of surface of skin. The pharmaceutical compound can pass through this channel into the human body for delivering the drug including the larger or small compound. The upper electrode  54  is called the electromagnetic electrode, and the lower electrode  56  is called the electroporation electrode. The architecture is shown in  FIG. 12 . In order to simplify the moving principle of the present invention, only one set of electrode is positioned in the upper electrode, and two sets of electrodes are positioned in the lower electrode. This combination is described by the architecture of electrodes of  FIG. 13  and the drive timing of  FIG. 14   
         [0061]     In order to describe the moving principle of the present invention, a single set of upper electrode (the electromagnetic electrode)  54  and two sets of lower electrode (electroporation electrodes) are detailed shown in  FIG. 13 .  
         [0000]     (I) The Drug with Positive Polarity  
         [0062]     When the polarity of pharmaceutical compound which is going to deliver the human body is positive, the time-varied electromagnetic field is produced if the drug is positioned between the upper electrode and the lower electrode and the time-varied voltage is applied on these two electrodes, so that the pharmaceutical compound has the kinetic energy moving toward the skin. For the lower electrode, due to the rotational electric field applied by the alternating voltage, an ion channel is formed in the surface of skin, so that the pharmaceutical compound is delivered into the human body more easily. For the combination set of the alternating electric field and the rotational alternating electric field on the patch, the various combinations are formed, depending on the number of upper electrode and lower electrode. In order to simplify the moving principle of the present invention, only one set of electrode is positioned in the upper electrode, and two sets of electrodes are positioned in the lower electrode. This combination is described by the architecture of electrodes of  FIG. 13  and the drive timing of  FIG. 14 . As shown in  FIG. 14 , each drive period has four states. There are the differences of two states t 0 ˜t 1  and t 2 ˜t 3  in four states. There is no voltage applied on the lower electrodes  561  and  562 . The polarities of other electrodes are not changed. The drive timings t 0 ˜t 1  and t 2 ˜t 3  are moving the same way. The lower electrode  561  in the electric field is changed into the lower electrode  562 , depending on the different state. According to the aforementioned, the movement ways of t 0 ˜t 2  and t 2 ˜t 4  are moving similar. In the following, the movement ways of t 0 ˜t 2  are only described.  
         [0000]     (I) State  1  (t=t 0 ˜t 1 )  
         [0063]     In this state, for the upper electrode  54  and the lower electrode  561 , the positive voltages are applied on their voltage levels, and the voltage level and the timing-varied are the same. The variations in the electric field and the magnetic field are not changed between these two electrodes. For the lower electrode  562 , the applied voltage is zero level of voltage. There is a variation of voltage between the lower electrode  562  and the upper electrode  54 . The variation of voltage is changed between these two electrodes, depending on the plane position of the electrodes  561  and  562 . The plane position of pharmaceutical compound on the lower electrode  561  and  562  is changed as three different areas, respectively, as shown in  FIGS. 15, 16  and  17 . In these figures, it can be found that, the vector of electric field is represented by the right-angled coordinate axis. The three different areas having the electric field profiles are analyzed as followings:  
         [0064]     (a) The force which is applied on the pharmaceutical compound by the component of electric field having xy coordinate plane, as shown in  FIG. 15 , when a pharmaceutical compound A is positioned on the xy coordinate plane of lower electrode  561  and  562 , a component of electric field is produced on this coordinate plane, and this component of electric field is profiled on the xy coordinate plane. The component of electric field caused by the lower electrode  562  to the upper electrode  54  is represented by the following equation (8). 
 
 {right arrow over (E)}   UB   ={right arrow over (E)}   xB ( x,y,t ) {right arrow over (i)}   x   +E   yB ( x,y,t ) {right arrow over (i)}   y    (8) 
 
 where {right arrow over (E)} UB  is the vector of electric field profile caused by the upper electrode  54  to the lower electrode  562 , E xB  is the component of {right arrow over (E)} UB  on x coordinate axis, E yB  is the component of {right arrow over (E)} UB  on y coordinate axis, and {right arrow over (i)} x  and {right arrow over (i)} y  are the unit vectors of the right-angled coordinate axis. 
 
         [0065]     After the relationship of electric field vector is obtained, the equation (8) is calculated according to the equation (5). The following relationship equation is obtained.  
                 (         ∂     E   yB         ∂   x       -       ∂     E   xB         ∂   y         )     ⁢           ⁢       i   ⇀     z       =       -     ⅆ     ⅆ   t         ⁢   B   ⁢       i   ⇀     z               (   9   )             
 
 where ∂E yB /∂x is taking x as the partial derivative of component of {right arrow over (E)} UB  on y axis, ∂E xB /∂y is taking y as the partial derivative of component of {right arrow over (E)} UB  on x axis, d/dt B is taking the differential of time by the magnetic flux when the electric field is changed. 
 
         [0066]     According to the equation (9), a magnetic field {right arrow over (B)} is induced by the time-varied electric field. When the pharmaceutical compound is positioned in the electric filed and the magnetic field inducted by the electric field, the pharmaceutical compound produces a force {right arrow over (F)} e1  of electric field by the electric field of upper electrode  54 , thereby making the pharmaceutical compound downwardly moving with a velocity v. When this force {right arrow over (F)} e1  affects the moving pharmaceutical compound, the pharmaceutical compound is subjected to a force {right arrow over (F)} m1  in the magnetic field induced by the electric field. The magnitude and direction of this force {right arrow over (F)} m1  of magnetic field are determined by the equation (3). According to the above-mentioned analysis, it found that the pharmaceutical compound is subjected to the force {right arrow over (F)} e1  of electric field and the force {right arrow over (F)} m1  of magnetic field, represented by the equation (4), a force {right arrow over (F)} c1  is interacted with these two forces. The magnitude and direction of this force {right arrow over (F)} e1  are the magnitude and direction of the vectors of {right arrow over (F)} e1  and {right arrow over (F)} m1  plus each other, as shown in  FIG. 18 . In  FIG. 18 , it is seen that the direction of force {right arrow over (F)} c1  is pointed toward the directions of lower electrode  561  and  562 . If the bottom of lower electrode  561  and  562  is positioned on the skin, a force {right arrow over (F)} c1  is produced. According to the above-mentioned analysis, a force is produced by the electric field profiled on the xy coordinate plane, thereby having the pharmaceutical compound with the kinetic energy moving towards the skin.  
         [0067]     (b) The force which is applied on the pharmaceutical compound by the component of electric field having xz coordinate plane, as shown in  FIG. 16 , when a pharmaceutical compound B is positioned on the xz coordinate plane of lower electrode  561  and  562 , a component of electric field is produced on this coordinate plane, and this component of electric field is profiled on the xz coordinate plane. The component of electric field caused by the lower electrode  562  from the upper electrode  54  is represented by the following equation (10). 
 
 {right arrow over (E)}   UB   =E   xB ( x,y,t ){right arrow over (i)} x   +E   zB ( x,y,t ){right arrow over (i)} z    (10) 
 
 where {right arrow over (E)} UB  is the vector of electric field profile caused by the upper electrode  54  to the lower electrode  562 , E xB  is the component of {right arrow over (E)} UB  on x coordinate axis, E yB  is the component of {right arrow over (E)} UB  on y coordinate axis, and {right arrow over (i)} x  and {right arrow over (i)} y  are the unit vectors of the right-angled coordinate axis. 
 
         [0068]     After the vector relationship of electric field vector is obtained, the equation (10) is calculated according to the equation (5). The following relationship equation is obtained.  
                 (         ∂     E   xB         ∂   z       -       ∂     E   zB         ∂   x         )     ⁢           ⁢       i   ⇀     y       =       -     ⅆ     ⅆ   t         ⁢   B   ⁢       i   ⇀     y               (   11   )             
 
 where ∂E xB /∂z is taking z as the partial derivative of component of {right arrow over (E)} UB  on x axis, ∂E zB /∂y is taking x as the partial derivative of component of {right arrow over (E)} UB  on z axis, d/dt B is taking the differential of time by the magnetic flux when the electric field is changed. 
 
         [0069]     According to the equation (11), a magnetic field {right arrow over (B)} is induced by the time-varied electric field. When the pharmaceutical compound is positioned in the electric filed and the magnetic field inducted by the electric field, the pharmaceutical compound produces a force {right arrow over (F)} e2  of electric field due to the electric field of upper electrode  54 , thereby having the pharmaceutical compound with a velocity v downwardly moving. When the force {right arrow over (F)} e2  affects the moving pharmaceutical compound, a force {right arrow over (F)} m2  is produced in the magnetic field induced by the electric field. The magnitude and direction of this force {right arrow over (F)} m2  of magnetic field are determined by the equation (3). According to the above-mentioned analysis, it found that the pharmaceutical compound is subjected to the force {right arrow over (F)} e2  of electric field and the force {right arrow over (F)} m2  of magnetic field, represented by the equation (4), a force {right arrow over (F)} c2  is interacted with these two forces. The magnitude and direction of this force {right arrow over (F)} c2  are the magnitude and direction of the vectors of {right arrow over (F)} e2  and {right arrow over (F)} m2  plus each other, as shown in  FIG. 19 , which is shown that the resulting force {right arrow over (F)} c2  is moving toward the skin. Thus, according to the above-mentioned analysis, a force is produced by the electric field profiled on the xy coordinate plane, thereby having the pharmaceutical compound with the kinetic energy moving toward the skin.  
         [0070]     (c) The force which is applied on the pharmaceutical compound by the component of electric field having xy, yz and, zx coordinate planes, as shown in  FIG. 17 , when a pharmaceutical compound C is positioned on the xyz coordinate plane of lower electrode  561  and  562 , a component of electric field is produced on this coordinate plane, and this component of electric field comprises three components x, y and z. The component of electric field caused by the lower electrode  562  from the upper electrode  54  is represented by the following equation (12). 
 
 {right arrow over (E)}   UB   =E   xB ( x,y,t ) {right arrow over (i)}   x   +E   yB ( x,y,t ) {right arrow over (i)}   y   +E   zB ( x,y,t ) {right arrow over (i)}   z    (12) 
 
 where {right arrow over (E)} UB  is the vector of electric field profile caused by the upper electrode  54  to the lower electrode  562 , E xB  is the component of {right arrow over (E)} UB  on x coordinate axis, E yB  is the component of {right arrow over (E)} UB  on y coordinate axis, E zB  is the component of {right arrow over (E)} UB  on z coordinate axis and, {right arrow over (i)} x , {right arrow over (i)} y  and {right arrow over (i)} z  are the unit vectors of the right-angled coordinate axis. 
 
         [0071]     After the vector relationship of electric field vector is obtained, the equation (12) is calculated according to the equation (5). The following relationship equation is obtained.  
                   (         ∂     E   zB         ∂   y       -       ∂     E   yB         ∂   z         )     ⁢           ⁢       i   ⇀     x       +       (         ∂     E   xB         ∂   z       -       ∂     E   zB         ∂   x         )     ⁢           ⁢       i   ⇀     y       +       (         ∂     E   yB         ∂   x       -       ∂     E   xB         ∂   z         )     ⁢           ⁢       i   ⇀     z         =         -     ⅆ     ⅆ   t         ⁢   B   ⁢       i   ⇀     x       -       ⅆ     ⅆ   t       ⁢   B   ⁢       i   ⇀     y       -       ⅆ     ⅆ   t       ⁢   B   ⁢       i   ⇀     z                 (   13   )             
 
         [0072]     Where ∂E zB /∂y is taking y as the partial derivative of component of {right arrow over (E)} UB  on z axis, ∂E yB /∂z is taking z as the partial derivative of component of {right arrow over (E)} UB  on y axis, ∂E xB /∂z is taking z as the partial derivative of component of {right arrow over (E)} UB  on x axis, ∂E zB /∂y is taking x as the partial derivative of component of {right arrow over (E)} UB  on z axis, ∂E xB /∂y is taking x as the partial derivative of component of {right arrow over (E)} UB  on y axis, ∂E xB /∂y is taking y as the partial derivative of component of {right arrow over (E)} UB  on x axis, d/dt B is taking the differential of time by the magnetic flux when the electric field is changed.  
         [0073]     According to the equation (13), a magnetic field {right arrow over (B)} is induced by the time-varied electric field. When the pharmaceutical compound is positioned in the electric filed and the magnetic field inducted by the electric field, the pharmaceutical compound produces a force {right arrow over (F)} E  of electric field due to the electric field of upper electrode  54 , thereby having the pharmaceutical compound with a velocity v downwardly moving. Thus, there are the components of x, y, and z coordinate in the magnitude field according to the equation (15). The forces of magnetic field comprise three forces of components {right arrow over (F)} mx , {right arrow over (F)} my , and {right arrow over (F)} mz , respectively. These three forces of components are interacted with the force {right arrow over (F)} E  of electric field. When interacting with the force {right arrow over (F)} E , the force {right arrow over (F)} mx  is parallel with the moving direction v (on the x coordinate axis) due to the direction of magnetic field (on the x coordinate axis), represented by the equation (3). The force {right arrow over (F)} mx  will not be produced. Therefore, the pharmaceutical compound is only subjected to the force {right arrow over (F)} E . Two forces {right arrow over (F)} my  and {right arrow over (F)} mz  are perpendicular to the force {right arrow over (F)} E , thereby having the pharmaceutical compound with a force to move toward the skin. This force is conduced as same as the component of electric field of the above-mentioned charged particle on xy and xz coordinate. The forces profiled on xyz coordinate axis to the pharmaceutical compound are shown in the total resulting force {right arrow over (F)} C3  of the vector diagram of  FIG. 20 . In the vector diagram, if {right arrow over (F)} my (−{right arrow over (i)} y ) is equal to {right arrow over (F)} mz (−{right arrow over (i)} z ), these two forces are interacted with the force {right arrow over (F)} E ({right arrow over (i)} x ) to produce the force {right arrow over (F)} 1 ({right arrow over (i)} x , −{right arrow over (i)} y ) and the force {right arrow over (F)} 2 ({right arrow over (i)} x , −{right arrow over (i)} z ), respectively. In order to combine the force {right arrow over (F)} 1 ({right arrow over (i)} x ,−{right arrow over (i)} y ), {right arrow over (F)} 2 ({right arrow over (i)} x ,−{right arrow over (i)} z ), and {right arrow over (F)} E ({right arrow over (i)} x ) to a resulting force, the force {right arrow over (F)} 2 ({right arrow over (i)} x ,−{right arrow over (i)} z ) and {right arrow over (F)} E ({right arrow over (i)} x ) are combined to a resulting force {right arrow over (F)} E2 ({right arrow over (i)} x ,−{right arrow over (i)} z ), firstly. The force {right arrow over (F)} E2 ({right arrow over (i)} x , −{right arrow over (i)} z ) and {right arrow over (F)} 1 ({right arrow over (i)} x ,−{right arrow over (i)} y ) are combined to a total resulting force {right arrow over (F)} C3 . According to the vector diagram, the component direction of total resulting force {right arrow over (F)} C3  is toward the direction of the surface of skin. Therefore, the total resulting force {right arrow over (F)} C3  also causes the pharmaceutical compound to move toward the surface of skin.  
         [0074]     According to the above-mentioned analysis, in the state  1 , two-electrode structure comprises a force applied on the pharmaceutical compound, thereby having the pharmaceutical compound with a kinetic energy to move toward the direction of the skin.  
         [0000]     (1) State  2  (t=t 1 ˜t 2 )  
         [0075]     In this state, 0 voltage is respectively applied on the upper electrode  54  and the lower electrode  561  and  562 . There is no force applied on the pharmaceutical compound.  
         [0076]     As a result, an alternating voltage is applied by using two electrodes to obtain a force toward the direction of skin. The same effect is obtained while changing the number of upper electrode and lower electrode. Even, the treatment area of the entire patch can be increased. Or, the voltage applied on the electrode can be reduced on the same treatment area. Even, the treatment area of the entire patch can be increased. Or, the voltage applied on the electrode can be reduced on the same treatment area in order to obtain the same effect between the electrodes while using the fewer electrodes. The multi-electrode structure, which is shown in  FIG. 21 , comprises a single set of upper electrode (the electromagnetic field electrode)  54  and three sets of lower electrodes (electroporation electrode)  561 ,  562 , and  563 . The multi-electrode structure, which is shown in  FIG. 22 , comprises a single set of upper electrode (the electromagnetic field electrode)  54  and four sets of lower electrodes (electroporation electrode)  561 ,  562 ,  563  and  564 , and also uses the drive timing diagram shown in  FIGS. 23 and 24  in order to drive three sets of electroporation electrodes and four sets of electroporation electrodes, respectively. The combination way of n sets of electrodes will be conducted depending on the combination of electrodes.  
         [0000]     (II) The Drug with Negative Polarity  
         [0077]     When the polarity of pharmaceutical compound which is going to deliver the human body is negative, the alternating electromagnetic field is produced if the drug is positioned between the upper electrode and the lower electrode and the time-varied voltage is applied on these two electrodes, so that the pharmaceutical compound has the kinetic energy moving toward the skin. For the lower electrode, due to the rotational electric field applied by the alternating voltage, an ion channel is formed in the surface of skin, so that the pharmaceutical compound is delivered into the human body more easily. In order to simplify the moving principle of the present invention herein, only one set of electrode is positioned in the upper electrode, and two sets of electrodes are positioned in the lower electrode. This combination is described by the architecture of electrodes of  FIG. 13  and the drive timing of  FIG. 25 . As shown in  FIG. 25 , each drive period has four states. There are the differences of two states t 0 ˜t 1  and t 2 ˜t 3  in four states. There is no voltage applied on the lower electrode  561  and  562 . The polarities of other electrodes are not changed. The drive timings t 0 ˜t 1  and t 2 ˜t 3  are moving the same way. The lower electrode  561  in the electric field is changed into the lower electrode  562 , depending on the different state.  
         [0000]     (1) State  1  (t=t 0 ˜t 1 )  
         [0078]     In this state, for the upper electrode  54  and the lower electrode  561 , the negative voltages (−V) are applied on their voltage levels, and the voltage level and the timing-varied are the same. The variations in the electric field and the magnetic field are not changed between these tow electrodes. For the lower electrode  562 , the applied voltage is zero level of voltage. There is a variation of voltage between the lower electrode  562  and the upper electrode  54 , and there is a variation of alternating electric field. This variation of alternating electric field is changed between these two electrodes, depending on the plane position of the electrodes  561  and  562 . The plane position of the pharmaceutical compound on the lower electrode  561  and  562  is changed as three different areas, respectively, as shown in  FIGS. 26, 27  and  28 . In these Figures, it can be seen that the vector of electric field is represented by the right-angled coordinate axis. The three different areas having the electric field profiles are analyzed as followings:  
         [0079]     (a) The force which is applied on the pharmaceutical compound by the component of electric field having xy coordinate plane, as shown in  FIG. 26 , when a pharmaceutical compound A is positioned on the xy coordinate plane of lower electrode  561  and  562 , a component of electric field is produced on this coordinate plane, and this component of electric field is profiled on the xy coordinate plane. The component of electric field caused by the lower electrode  562  from the upper electrode  54  is represented by the following equation (14). 
 
 {right arrow over (E)}   BU   =E   xB ( x,y,t ) {right arrow over (i)}   x   +E   yB ( x,y,t ) {right arrow over (i)}   y    (14) 
 
 were {right arrow over (E)} BU  is the vector of electric field profile caused by the upper electrode  54  to the lower electrode  562 , E xB  is the component of {right arrow over (E)} BU  on x coordinate axis, E yB  is the component of {right arrow over (E)} BU  on y coordinate axis, and {right arrow over (i)} x  and {right arrow over (i)} y  are the unit vectors of the right-angled coordinate axis. 
 
         [0080]     After the relationship of electric field vector is obtained, the equation (14) is calculated according to the equation (15). The following relationship equation is obtained.  
                 (         ∂     E   yB         ∂   x       -       ∂     E   xB         ∂   y         )     ⁢           ⁢       i   ⇀     z       =       -     ⅆ     ⅆ   t         ⁢   B   ⁢       i   ⇀     z               (   15   )             
 
 where ∂E yB /∂x is taking x as the partial derivative of component of {right arrow over (E)} UB  on y axis, ∂E xB /∂y is taking y as the partial derivative of component of {right arrow over (E)} UB  on x axis, d/dt B is taking the differential of time by the magnetic flux when the electric field is changed. 
 
         [0081]     According to the equation (15), a magnetic field {right arrow over (B)} is induced by the time-varied electric field. When the pharmaceutical compound is positioned in the electric filed and the magnetic field induced by the electric field, the pharmaceutical compound produces a force {right arrow over (F)} e4  of electric field due to the electric field of upper electrode  54 , thereby having the pharmaceutical compound with a velocity v downwardly moving. When the force {right arrow over (F)} e4  affects the moving pharmaceutical compound, a force {right arrow over (F)} m2  is produced in the magnetic field induced by the electric field. The magnitude and direction of this force {right arrow over (F)} m2  of magnetic field are determined by the equation (3). According to the above-mentioned analysis, it found that the pharmaceutical compound is subjected to the force {right arrow over (F)} e3  of electric field and the force {right arrow over (F)} m4  of magnetic field, represented by the equation (4), a force {right arrow over (F)} c4  is interacted with these two forces. The magnitude and direction of this force {right arrow over (F)} c4  are the magnitude and direction of the vectors of {right arrow over (F)} e3  and {right arrow over (F)}m 3  plus each other, as shown in  FIG. 29 . In  FIG. 29 , it is seen that the direction of the force {right arrow over (F)} c4  is pointed toward the directions of lower electrode  561  and  562 . If the bottom of lower electrode  561  and  562  is positioned on the skin, a force {right arrow over (F)} c3  is produced. According to the above-mentioned analysis, a force is produced by the electric field profiled on the xy coordinate plane, thereby having the pharmaceutical compound with the kinetic energy moving towards the skin.  
         [0082]     (b) The force which is applied on the pharmaceutical compound by the component of electric field having xz coordinate plane, as shown in  FIG. 27 , when a pharmaceutical compound B is positioned on the xz coordinate plane of lower electrode  561  and  562 , a component of electric field is produced on this coordinate plane, and this component of electric field is profiled on the xz coordinate plane. The component of electric field caused by the lower electrode  562  from the upper electrode  54  is represented by the following equation (16). 
 
 {right arrow over (E)}   BU   =E   xB ( x,y,t ) {right arrow over (i)}   x   +E   zB ( x,y,t ) {right arrow over (i)}   z    (16) 
 
 where {right arrow over (E)} BU  is the vector of electric field profile caused by the upper electrode  54  to the lower electrode  562 , E xB  is the component of {right arrow over (E)} BU  on x coordinate axis, E zB  is the component of {right arrow over (E)} BU  on z coordinate axis, and {right arrow over (i)} x  and {right arrow over (i)} y  are the unit vectors of the right-angled coordinate axis. 
 
         [0083]     After the vector relationship of electric field vector is obtained, the equation (16) is calculated according to the equation (5). The following relationship equation is obtained.  
                 (         ∂     E   xB         ∂   z       -       ∂     E   zB         ∂   x         )     ⁢           ⁢       i   ⇀     y       =       -     ⅆ     ⅆ   t         ⁢   B   ⁢       i   ⇀     y               (   17   )             
 
 where ∂E xB /∂z is taking z as the partial derivative of component of {right arrow over (E)} BU  on x axis, ∂E zB /∂y is taking x as the partial derivative of component of {right arrow over (E)} BU  on z axis, d/dt {right arrow over (B)} is taking the differential of time by the magnetic flux when the electric field is changed. 
 
         [0084]     According to the equation (17), a magnetic fields {right arrow over (B)} is induced by the time-varied electric field. When the pharmaceutical compound is positioned in the electric filed and the magnetic field induced by the electric field, the pharmaceutical compound produces a force {right arrow over (F)} e5  of electric field due to the electric field of upper electrode  54 , thereby having the pharmaceutical compound with a velocity v downwardly moving. When the force {right arrow over (F)} e5  affects the moving pharmaceutical compound, a force {right arrow over (F)} m5  is produced in the magnetic field induced by the electric field. The magnitude and direction of this force {right arrow over (F)} m2  of magnetic field are determined by the equation (3). Therefore, when the pharmaceutical compound is subjected to the force {right arrow over (F)} e5  of electric field and the force {right arrow over (F)} m5  of magnetic field, represented by the equation (4), a force {right arrow over (F)} c4  is interacted with these two forces. The magnitude and direction of this force {right arrow over (F)} c4  are the magnitude and direction of the vectors of {right arrow over (F)} e5  and {right arrow over (F)} m5  plus each other, as shown in  FIG. 30 , which is shown that the resulting force {right arrow over (F)} c4  is moving toward the skin.  
         [0085]     (c) The force which is applied on the pharmaceutical compound by the component of electric field having xy, yz and zx coordinate planes, as shown in  FIG. 28 , when a pharmaceutical compound C is positioned on the xyz coordinate plane of lower electrode  561  and  562 , a component of electric field is produced on this coordinate plane, and this component of electric field comprises three components, x, y and z. The component of electric field caused by the lower electrode  562  from the upper electrode  54  is represented by the following equation (18). 
 
 {right arrow over (E)}   BU   =E   xB ( x,y,t ) {right arrow over (i)}   x   +E   yB ( x,y,t ) {right arrow over (i)}   y   +E   zB ( x,y,t ) {right arrow over (i)}   z    (18) 
 
 where {right arrow over (E)} BU  is the vector of electric field profile caused by the upper electrode  54  to the lower electrode  562 , E xB  is the component of {right arrow over (E)} BU  on x coordinate axis, E yB  is the component of {right arrow over (E)} BU  on y coordinate axis, E zB  is the component of {right arrow over (E)} BU  on z coordinate axis, and  x , {right arrow over (i)} y  and {right arrow over (i)} z  are the unit vectors of the right-angled coordinate axis. 
 
         [0086]     After the vector relationship of electric field vector is obtained, the equation (18) is calculated according to the equation (5). The following relationship equation is obtained.  
                   (         ∂     E   zB         ∂   y       -       ∂     E   yB         ∂   z         )     ⁢           ⁢       i   ⇀     x       +       (         ∂     E   xB         ∂   z       -       ∂     E   zB         ∂   x         )     ⁢           ⁢       i   ⇀     y       +       (         ∂     E   yB         ∂   x       -       ∂     E   xB         ∂   z         )     ⁢           ⁢       i   ⇀     z         =         -     ⅆ     ⅆ   t         ⁢   B   ⁢       i   ⇀     x       -       ⅆ     ⅆ   t       ⁢   B   ⁢       i   ⇀     y       -       ⅆ     ⅆ   t       ⁢   B   ⁢       i   ⇀     z                 (   19   )             
 
 where ∂E zB /∂y is taking y as the partial derivative of component of {right arrow over (E)} BU  on z axis, ∂E yB /∂z is taking z as the partial derivative of component of {right arrow over (E)} BU  on y axis, ∂E yB /∂z is taking z as the partial derivative of component of {right arrow over (E)} BU  on x axis, ∂E zB /∂y is taking y as the partial derivative of component of {right arrow over (E)} BU  on z axis, ∂E yB /∂x is taking x as the partial derivative of component of {right arrow over (E)} UB  on y axis, ∂E xB /∂y is taking y as the partial derivative of component of {right arrow over (E)} UB  on x axis, and d/dt B is taking the differential of time by the magnetic flux when the electric field is changed. 
 
         [0087]     According to the equation (19), a magnetic field {right arrow over (B)} is induced by the time-varied electric field. When the pharmaceutical compound is positioned in the electric filed and the magnetic field inducted by the electric field, the pharmaceutical compound produces a force {right arrow over (F)} E  of electric field due to the electric field of upper electrode  54 , thereby having the pharmaceutical compound with a velocity v downwardly moving. Thus, there are the components of x, y and z coordinate in the magnitude field according to the equation (19). The forces of magnetic field comprise three forces of components {right arrow over (F)} mx , {right arrow over (F)} my  and {right arrow over (F)} mz , respectively. These three forces of components are interacted with the force {right arrow over (F)} E  of electric field. When interacting with the force {right arrow over (F)} E , the force {right arrow over (F)} mx  is parallel with the moving direction v (on the x coordinate axis) due to the direction of magnetic field (on the x coordinate axis), represented by the equation (3). The force {right arrow over (F)} mx  will not be produced. Therefore, the pharmaceutical compound is only subjected to the force {right arrow over (F)} E . Two forces {right arrow over (F)} my  and {right arrow over (F)} mz  are perpendicular to the force {right arrow over (F)} E , thereby having pharmaceutical compound with a force to move toward the skin. This force is conduced as same as the component of electric field of the above-mentioned charged particle on xy and xz coordinate. The forces profiled on xyz coordinate axis to the pharmaceutical compound are shown in the total resulting force {right arrow over (F)} C6  of the vector diagram of  FIG. 31 . In the vector diagram, if {right arrow over (F)} my (−{right arrow over (i)} y ) is equal to {right arrow over (F)} mz (−{right arrow over (i)} y ), these two forces are interacted with the force {right arrow over (F)} E ({right arrow over (i)} x ) to produce the force {right arrow over (F)} 3 ({right arrow over (i)} x , −{right arrow over (i)} y ) and the force {right arrow over (F)} 4 ({right arrow over (i)} x , −{right arrow over (i)} z ), respectively. In order to obtain a resulting force {right arrow over (F)} C6 , the force {right arrow over (F)} 3 ({right arrow over (i)} x ,−{right arrow over (i)} y ) and {right arrow over (F)} E ({right arrow over (i)} x ) are combined to a resulting force {right arrow over (F)} E3 ({right arrow over (i)} x ,{right arrow over (i)} y ), firstly. The force {right arrow over (F)} E3 ({right arrow over (i)} x ,{right arrow over (i)} y ) and {right arrow over (F)} 4 ({right arrow over (i)} x ,{right arrow over (i)} y ) are combined to a total resulting force {right arrow over (F)} C6 . According to the vector diagram, the component direction of total resulting force {right arrow over (F)} C6  is toward the direction of the surface of skin. Therefore, the total resulting force {right arrow over (F)} C6  also causes the pharmaceutical compound to move toward the surface of skin.  
         [0088]     According to the above-mentioned analysis, in the state  1 , two-electrode structure comprises a force applied on the pharmaceutical compound, thereby having the pharmaceutical compound with a kinetic energy to move toward the direction of the skin.  
         [0000]     (2) State  2  (t=t 1 ˜t 2 )  
         [0089]     In this state, 0 voltage is respectively applied on the upper electrode 54 and the lower electrode  561  and  562 . There is no force applied on the pharmaceutical compound. As a result, the drugs with positive polarity and negative polarity or neutrality have the same function and effect. The various combination ways are used, and the details are omitted herein. The present invention provides an electric energy auxiliary device of transdermal drug delivery patch with a multi-electrode structure having drug delivery efficiency of iontophoresis, electroporation, and natural diffusion in order to provide the strongly thrust by using two-electrode structure to deliver the pharmaceutical compounds into the human body readily, not being subject to the size and hydrophile of the pharmaceutical compounds so as to improve effectiveness of drug delivery. While the invention has been particularly shown and described with reference to the preferred embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made without departing from the spirit and scope of the invention.