Technical Field

The present invention relates to a method of and apparatus for biasing magnetic material. The invention has application for example to electrical devices such as transformers and inductors.

Background Art

The characteristic of magnetically soft material such as silicon steel, ferrite or the like is as sliown by the hysteresis loop and saturation magnetization curve in Fig. 2. In this drawing, B is the magnetic flux density, Bm is the saturation magnetic flux density, Br is the residual magnetic flux density, H is the magnetizing force. He is the coercive force and Hs is the saturation magnetizing force. As is apparent from the saturation magnetization curve shown in Fig. 2, even if a magnetizing force H (designated by the product of current in a winding and the number of turns of the winding), which is in excess of a predetermined amount, is provided to the magnetic material, the magnetic flux density B within the magnetic material will not exceed a predetermined amount Bm, due to the magnetic saturation. The value Bm is determined by the property of the material and the configuration of the magnetic material, gaps in a magnetic path and the like. The higher the saturation value Bm is, the more miniaturized can be a transformer, or the more miniaturized can be an inductor which can realize a predetermined inductance value.

In the case where a current flows or a voltage is applied intermittently to one end of a winding wound about a magnetic core, the magnetic material fulfills its function in a range from the

saturation magnetic flux density Bm to the residual magnetic flux density Br in Fig. 2.

However, as is apparent from Fig. 2, as a property of magnetic material, the magnetic flux density thereof can vary within a range from + Bm to - Bm. As shown in Fig. 3, a magnetic core 10 with magnetic polarity has been devised based on this fact. The core has a permanent magnet 12 which is inserted into a magnetic path such that the magnetic flux density obtained when the magnetizing force H is "0", that is the residual magnetic flux density Br, exhibits a negative value. Thereby it spreads substantially the usable range of the magnetic flux density. Thus, the combination of the magnetic core with a permanent magnetic permits a reduction in utilizing volume of the magnetic material and hence the miniaturization of the apparatus.

However, a biasing method or apparatus which uses a permanent magnet for magnetically biasing magnetic material (such as the magnetic core 10) has the following disadvantages: the apparatus is expensive, the bias level is fixed because the bias is applied by a permanent magnet, and the magnetic property of the permanent magnet deteriorates with long term usage.

Disclosure of the Invention

It is an object of the present invention to provide a method and apparatus for biasing magnetic material in which the above mentioned drawbacks are substantially overcome.

According to one aspect of the invention there is provided a method of magnetically biasing a magnetic core of an electrical device which includes a first coil in operative relation to said core, characterized by the following steps of providing a second coil in operative relation to said core and

associated operating circuitry for said second coil, said operating circuitry including first and second switching means, and applying a voltage across said first coil to produce a voltage across said second coil, the voltage produced across said second coil serving to operate said first switching means which is contained in an energizing circuit for said second switching means, and the operation of said first switching means serving to operate said second . switching means so as to connect a voltage source to said second coil, whereby a magnetic field is generated which acts to prevent saturation of said core.

According to another aspect of the invention there is provided a transformer apparatus including a primary winding having input means associated therewith, a secondary winding having output means associated therewith, and a magnetic core operatively associated with said primary and secondary windings, characterized by an auxiliary winding operatively associated with said magnetic core and operable to decrease the magnetic flux density of said core, first switching means having first operating means associated therewith, said first operating means being coupled to said auxiliary winding, and second switching means having associated therewith second operating means which includes said first switching means, said second switching means being operable to connect said output means of said secondary winding to said auxiliary winding, whereby the application of an appropriate voltage to said input means of said primary winding produces voltages across said output means of said secondary winding and across said auxiliary winding, the voltage across said output means being greater than that across said auxiliary winding, and the voltage across said auxiliary winding causing operation of said first switching means, which

in turn causes operation of said second switching means to cause said output means to be connected to said auxiliary winding so as to bias the magnetic core to prevent saturation thereof.

It should be understood that a method and apparatus in accordance with the invention each enable the usable range of the magnetic flux density to be spread without use of a special core so as to reduce the utilizing volume of the magnetic material, thereby enabling the miniaturization of the apparatus.

It should further be understood that in a method and apparatus in accordance with the invention, in addition to a conventional magnetic core and main winding, an auxiliary winding is provided which is so constructed as to decrease the magnetic flux which is generated in a magnetic path by- -the main winding in a predetermined amount in synchronism with an increase in said magnetic flux during the. time that said magnetic flux is increasing, to prevent the magnetic saturation of the magnetic material of the magnetic core.

Brief Description of the Drawings

One embodiment of the invention will now be described by way of example with reference to the accompanying drawings, in which:

Fig. 1 is a circuit diagram of a transformer apparatus according to the present invention;

Fig. 2, previously referred to, shows the saturation magnetization curves (B-H magnetization curves) and hysteresis loop of magnetic material;

Fig. 3, previously referred to, is a diagram of a magnetic core arrangement incorporating a permanent magnet; and

Fig. 4 is a diagram showing a change of magnetic flux density within the magnetic core of the apparatus of Fig. 1.

Best Mode for Carrying Out the Invention

Next, the present invention will be described with reference to the accompanying drawings.

Fig. 1 is a circuit diagram according to an embodiment of the present invention which is applied to a transformer. In Fig. 1, when an input voltage with a waveform shown in the drawing is applied across the main winding Nl, a voltage corresponding to ti /n-i of the input voltage in magnitude and having the same waveform as the input voltage is produced between the terminals of a secondary winding N3, where n^ and n3 are the number of turns of the windings Nl and N3 respectively. Numeral 2 denotes a magnetic core. The condition under which the core 2 is not saturated is determined by the following equation (1): ni > V x tl x ιo 10 (1)

A x ΔB where V is the maximum input voltage (volts), tl is the duration of each positive input voltage pulse applied to the winding Nl (seconds), A is the minimum sectional area in the magnetic path of the core 2 (mm ² ), and ΔB is the usable range of the magnetic flux density, that is, Bm - Br (gauss).

The equation (1) indicates that the relation between the number of turns n^ of the main winding Nl and the sectional area A in the magnetic path of the core 2 to prevent the core from being saturated is determined by ΔB, that is, a difference between the saturation magnetic flux density Bm and the residual magnetic flux density Br of the core 2, on condition that the input voltage and the duration time tl of each input voltage pulse are constant. Thus, a large ΔB can ensure the use of the core 2 with no saturation, even when the number of turns of the main winding is further reduced or the sectional area A in the magnetic path of the core 2 is further decreased. Taking notice of this point, in the magnetic core with

magnetic polarity shown in Fig. 3, the magnetic material is biased magnetically to decrease the residual magnetic flux density Br to a negative value with the use of the permanent magnet to increase the value of ΔB. On the other hand, in the present invention, the magnetic material is biased magnetically by a demagnetizing winding (auxiliary winding) N2 which is operative to demagnetize the magnetic flux density through the magnetic material in synchronism with the waveform of the input voltage applied across the main winding Nl to reduce the residual magnetic flux density Br to a negative value.

Next, the operation of the embodiment shown in Fig. 1 will be described.

The windings N3 and N2 are wound about the magnetic core in such- manner that during the- time that the input voltage is being applied across the main winding Nl (term tl), a voltage, in -a direction causing the forward bias of a diode D2 and the reverse bias of a diode D3 connected as shown in Fig.-l, is induced across the output winding N3. Also, a voltage, in a direction to turn on a transistor Tr2, is induced across the auxiliary winding N2. The inductor LI shown in Fig. 1 is a smoothing inductor.

Now, in response to a positive input voltage pulse applied across the main winding Nl, a voltage Eo is developed across a capacitor Cl by the winding N3. Also, a voltage is induced across the auxiliary winding N2, and the emitter-base of the transistor Tr2 is forward biased by resistors Rl and R2 so that the transistor Tr2 is in the "on" state. When the transistor Tr2 is turned on, base current is supplied through a resistor R3 to a transistor Trl to turn the transistor Trl on and then the voltage Eo is applied to the winding N2. In this case, if the voltage Eo exceeds the value of V * n2/ ]_ (where 2 is the number of turns of the auxiliary winding N2), a current 1^2

flows through the winding N2 in a direction to decrease the exciting current in the winding Nl. The magnetizing current IN2 is always maintained constant by a circuit arrangement consisting of the transistor Trl, a resistor R4, and a Zener diode Dl (Zener voltage Vz) as shown in Fig. 1. The relation thereof is expressed by the following equation (2): VBE ^{+ X} N2 ^* R4 = VZ ,

Therefore, 1^2 = Va ~ VBS (constant) .... (2)

R4 (VgE is the base-emitter voltage on the transistor Trl. ) As has been described above, in the present invention, the circuit arrangement in which the Zener diode Dl is used maintains the demagnetizing current Iu2 constant during the period of time tl, so that the exciting current in the main winding Nl is not affected. That is, the magnetic flux density in the core 2 is demagnetized by the predetermined amount always during the time tl. Supposing that the demagnetized amount is designated by ΔB1, the following equation (3) is established:

ΔB1 = y.H - M ' n ₂ ' IN2 < ³ )

(wherβ . is the magnetic permeability of magnetic material)

As is apparent from the above description, the present invention is constructed such that the voltage Eo exceeds the voltage induced by the auxiliary winding N2 and the demagnetizing current 1^2 is maintained constant by the circuit in which the Zener diode Dl is used, by which the magnetic flux density in the core 2 is demagnetized by the predetermined amount ΔB1 to prevent the magnetic saturation of the core 2.

Next, the time t2 during which no voltage is applied across the winding Nl will be described. The

transistor Tr2 is in the off state during the period ^' of time t2, so that the transistor Trl is also turned off and hence no current flows through the winding N2. The core 2 is not demagnetized in the absence of the demagnetizing current 1^2 i ⁿ the winding N2, so that the magnetic flux density of the core 2 instantaneously increases upon the commencement of the time period t2. However, since no voltage is applied across the winding Nl, even a saturated core 2 causes no problem.

Fig. 4 shows a change in the magnetic- flux density in the core 2. The. magnetic flux density in the magnetic material is demagnetized by the amount M.' ' IN derived from the equation (3) during the time tl, so that the saturation point is substantially raised by the amount corresponding thereto.

The present invention can apply to an inductor in the same manner as it is applied to a transformer with the exception that an external D-C voltage source corresponding to .the voltage Eo in Fig. 1 is needed.

As has been described above, according to the present invention, the addition of the auxiliary winding about the magnetic core and the simple circuit makes possible the miniaturization of a magnetic device and a reduction of the number of turns of the main winding. Under given working conditions, the present invention which is applied to a transformer or an inductor realized a reduction of about 30% in volume of the magnetic material as compared to conventional transformers or inductors which use magnetic material that is not biased magnetically.