This application is a national stage application of PCT/JP2016/057011, which claims priority to Japanese Application No. 2015-054362, both of which are incorporated herein by reference.
The present invention relates to a loop antenna which can contribute to an increase of an area of a radio system using a magnetic field.
A radio system utilizing a magnetic field has been conventionally proposed. Unlike radio waves, the magnetic field hardly interacts with human bodies and dielectric materials, and is thus advantageous in forming a definite radio area which is undisrupted by human bodies and obstacles. Moreover, the distance attenuation characteristic of a radio wave is 20 dB/dec., while the distance attenuation characteristic of a magnetic field is 60 dB/dec. Thus, the magnetic field is suitable in the case of definitely defining a radio area boundary.
However, the distance attenuation characteristic (60 dB/dec.) of the magnetic field which is steeper than that of the radio wave is a disadvantageous factor in the case of increasing the radio area. Conventionally, in order to increase the area of the radio system using the magnetic field, a current supplied from a transmitter has to be increased.
The present invention has been made in view of the problems described above and an objective thereof is to provide a loop antenna which can contribute to an increase of an area of a radio system using a magnetic field.
In order to solve the problems described above, a loop antenna in a first aspect of the present invention includes a main loop which is an open loop connected to a signal source or a reception circuit; and an amplification loop which is a closed loop having a same shape as the main loop, and the main loop and the amplification loop are arranged on a same surface of a flat substrate formed of an insulator.
A loop antenna in a second aspect of the present invention includes: a main loop which is an open loop connected to a signal source or a reception circuit; and an amplification loop which is a closed loop having a same shape as the main loop, and the main loop and the amplification loop are arranged on different surfaces of a flat substrate formed of an insulator or on different flat substrates in a structure in which a plurality of flat substrates are stacked one on top of another.
In the loop antenna of the present invention, in the case where the signal source is used, a current sufficiently larger than a current flowing through the main loop can be accumulated in the amplification loop. As a result, a large magnetic field can be generated.
In the loop antenna of the present invention, in the case where the reception circuit is used, an effect in which a large current is accumulated in the amplification loop in the reception of the magnetic field allows the main loop to receive a reception current larger than that in the case where no amplification loop is used.
As result, the loop antenna of the present invention can contribute to an increase of an area of a radio system using a magnetic field.
Embodiments of the present invention are described below with reference to the drawings.
The loop antenna is a resonant loop antenna and includes a main loop 1 and an amplification loop 2.
The main loop 1 is formed on a flat substrate (not illustrated) formed of an insulator, includes terminals T, T for connection to a signal source 5 or a reception circuit (not illustrated), and is an open loop. The number of turns is one.
The amplification loop 2 is formed very close to the main loop 1, on the same surface of the flat substrate on which the main loop 1 is formed. The amplification loop 2 includes no terminals and is a closed loop. The number of turns is one. The amplification loop 2 is arranged inside the main loop 1.
The distance d between the main loop 1 and the amplification loop 2 is, for example, equal to or smaller than one-tenth of a square root of the area of a region surrounded by the main loop 1 or the amplification loop 2. A resistance R2 and a capacitance C2 are connected to the amplification loop 2 in series.
When an alternating current (AC current) I1 is supplied from the signal source 5 to the main loop 1, mutual inductance between the main loop 1 and the amplification loop 2 causes an AC current I2 to flow through the amplification loop 2. Generally, when R2 is smaller than R1, I2 is larger than I1. An area of a magnetic field generated by the loop antenna can be thus increased.
I2 depends on multiple factors such as a frequency, R1, R2, C1, C2, an internal resistance R0 of the signal source 5, and the shape of the loop. Accordingly, it is desirable to maximize I2 by adjusting R1, R2, C1, and C2.
Note that, although
In this case, a magnetic field received from the outside causes a large AC current I2 to be accumulated in the amplification loop 2. Moreover, since there is mutual inductance, the AC current I1 flowing through the main loop 1 is larger than that in the case where there is no amplification loop 2. I1 can be maximized by setting R1, R2, C1, and C2 depending on the frequency, the shape of the loop, and the like. The area of the magnetic field can be thereby increased also for the other party.
Thus, the loop antenna in the first embodiment can increase the area of the radio system utilizing the magnetic field.
Note that the amplification loop 2 may be arranged outside the main loop 1. In other words, the loops are arranged such that one loop includes the other loop therein. The same applies to the embodiments to be described later. As illustrated in
When a desired current or area can be obtained, one or plurality of R1, R2, C1, and C2 may not be used. The same applies to the embodiments to be described later.
In the first embodiment, the number of turns is one in both of the main loop 1 and the amplification loop 2. However, in the second embodiment, the number of turns is three in both loops. Other configurations are the same as those in the first embodiment. The amplification loop 2 is arranged inside the main loop 1.
The number of turns in the present invention is arbitrary and any number of turns is effective. The number of turns may vary between the main loop 1 and the amplification loop 2. However, when the number of turns is two or more, equalizing the number of turns in the main loop 1 and the number of turns in the amplification loop 2 can increase the mutual inductance and thus increase the effect of amplifying the current. Accordingly, it is preferable to equalize the number of turns in the main loop 1 and the number of turns in the amplification loop 2.
In the first and second embodiments, the main loop 1 and the amplification loop 2 are provided on the same flat surface of the flat substrate and the amplification loop 2 is arranged inside or outside the main loop 1 to be provided close thereto.
In the third embodiment, the main loop 1 is formed on a front surface of the flat substrate and the amplification loop 2 is formed on a back surface of the same flat substrate. Other configurations are the same as those in the first embodiment. The main loop 1 and the amplification loop 2 only needs to be formed separately on the different surfaces (front and back surfaces) of the flat substrate. Accordingly, the configuration may be such that the main loop 1 is formed on the back surface of the flat substrate and the amplification loop 2 is formed on the front surface of the same flat substrate.
Forming the main loop 1 and the amplification loop 2 respectively on the front and back surfaces of the same flat substrate allows the main loop 1 and the amplification loop 2 to have the same shape and also to be provided close to each other. In this case, the main loop 1 and the amplification loop 2 can have the same shape and the same size, that is exactly the same shape. In this case, the distance between the main loop 1 and the amplification loop 2 is substantially equal to the thickness of the flat substrate. The distance is equal to or smaller than one-tenth of a square root of the area of a region surrounded by the main loop 1 or the amplification loop 2.
Since the main loop 1 and the amplification loop 2 have the same shape, it is possible to achieve the magnetic coupling coefficient close to 1 between the main loop 1 and the amplification loop 2 and increase the mutual inductance. Accordingly, larger I2 can be obtained relative to constant I1 when the signal source 5 is used, and larger I1 can be obtained relative to constant I2 when the reception circuit is used. In other words, the area of the magnetic field can be increased.
Note that, in a structure in which flat substrates are stacked one on top of another, the main loop 1 and the amplification loop 2 may be arranged respectively on different flat substrates. In this case, the distance between the main loop 1 and the amplification loop 2 is substantially equal to any integral multiple (single, double, . . . ) of the thickness of each flat substrate. The distance is equal to or smaller than one-tenth of a square root of the area of a region surrounded by the main loop 1 or the amplification loop 2.
The fourth embodiment has a configuration in which the number of turns is three in the loop antenna of the third embodiment. Other configurations are the same as those in the third embodiment.
As illustrated in
In the fourth embodiment, the main loop 1 and the amplification loop 2 are arranged, for example, on the different surfaces of the same flat substrate. Accordingly, the main loop 1 and the amplification loop 2 can be provided close to each other even when the number of turns in each of the main loop 1 and the amplification loop 2 is large. The same applies to the case where the main loop 1 and the amplification loop 2 are arranged on different flat substrates in the structure in which flat substrates are stacked one on top of another.
Thus, the mutual inductance between the main loop 1 and the amplification loop 2 does not decrease and the area of the magnetic field can be increased. This effect can be increased by increasing the number of turns.
Equalizing the number of turns in the main loop 1 and the number of turns in the amplification loop 2 can further increase the mutual inductance and increase the area of the magnetic field.
The loop antenna in a fifth embodiment is one in which the capacitances connected to the main loop 1 and the amplification loop 2 are optimized. Other configurations are the same as those in the first to fourth embodiments.
For example, the frequency f of a signal generated by the signal source 5 is 10 MHz, the resistance R1 connected to the main loop 1 is 25Ω, the resistance R2 connected to the amplification loop 2 is 1Ω, and the internal resistance R0 of the signal source 5 is 25Ω. In other words, the resistance R2 is smaller than the sum of the resistance R1 and the internal resistance R0.
The main loop 1 and the amplification loop 2 both have the same self-inductance L of 1 pH.
Since the self-inductance of a loop depends on the geometric shape thereof, the self-inductance of the main loop 1 and the self-inductance of the amplification loop 2 can be easily equalized by forming the main loop 1 and the amplification loop 2 in the same geometric shape.
When I2 is simulated under the aforementioned conditions with the capacitances C1 and C2 being variables, the result of
Meanwhile, when the aforementioned parameters are substituted into the following formulae:
C1=31.56 [pF] and C2=222.09 [pF] are obtained.
Accordingly, connecting C1 and C2 with the values calculated from these formulae to the main loop 1 and the amplification loop 2 can maximize I2 and provide the maximum amplification effect.
As illustrated in
Number | Date | Country | Kind |
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2015-054362 | Mar 2015 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2016/057011 | 3/7/2016 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2016/147934 | 9/22/2016 | WO | A |
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