7.3.1 Inductive Sensing

An AC current flowing through a coil will generate an AC magnetic field. If a conductive material, such as a metal target, is brought into the vicinity of the coil, this magnetic field will induce circulating currents (eddy currents) on the surface of the target. These eddy currents are a function of the distance, size, and composition of the target. The eddy currents then generate their own magnetic field, which opposes the original field generated by the coil. This mechanism is best compared to a transformer, where the coil is the primary core and the eddy current is the secondary core. The inductive coupling between both cores depends on distance and shape. Hence the resistance and inductance of the secondary core (eddy current), shows up as a distant dependent resistive and inductive component on the primary side (coil). The figures(Figure 5 to Figure 8) below show a simplified circuit model.

Figure 5. Inductor With A Metal Target

Eddy currents generated on the surface of the target can be modeled as a transformer as shown in Figure 6. The coupling between the primary and secondary coils is a function of the distance and the conductor’s characteristics. In Figure 6, the inductance Ls is the coil’s inductance, and Rs is the coil’s parasitic series resistance. The inductance L(d), which is a function of distance d, is the coupled inductance of the metal target. Likewise, R(d) is the parasitic resistance of the eddy currents and is also a function of distance.

Figure 6. Metal Target Modeled As L And R With Circulating Eddy Currents

Generating an alternating magnetic field with just an inductor will consume a large amount of power. This power consumption can be reduced by adding a parallel capacitor, turning it into a resonator as shown in Figure 7. In this manner the power consumption is reduced to the eddy and inductor losses Rs+R(d) only.

Figure 7. LC Tank Connected To Oscillator

The LDC1051 doesn’t measure the series resistance directly; instead it measures the equivalent parallel resonance impedance Rp (see Figure 8). This representation is equivalent to the one shown in Figure 8, where the parallel resonance impedance Rp(d) is given by:

Equation 1.

Figure 8. Equivalent Resistance Of Rs in Parallel With LC Tank

Figure 9 below shows the variation in Rp as a function of distance for a 14mm diameter PCB coil (Sensor Details:Table 16). The target in this example is a section of a 2mm thick stainless steel disk.

Figure 9. Typical Rp vs Distance With 14mm PCB Coil

7.3.2 Measuring Rp with LDC1051

The LDC1051 supports a wide range of LC combinations, with oscillation frequencies ranging from 5kHz to 5MHz and Rp ranging from 798Ω to 3.93MΩ. This range of Rp can be viewed as the maximum input range of an ADC. As illustrated in Figure 9, the range of Rp is typically much smaller than the maximum input range supported by the LDC1051. To get better resolution in the desired sensing range, the LDC1051 offers a programmable input range through the Rp_MIN and Rp_MAX registers. Refer to Calculation of Rp_MIN and Rp_MAX below for how to set these registers.

When the sensor’s resonance impedance Rp drops below the programed Rp_MIN, the LDC’s Rp output will clip at its full scale output. This situation could, for example, happen when a target comes too close to the coil.

Figure 10. Transfer Characteristics Of LDC1051 With Rp_MIN= 1.347 kΩ And Rp_MAX= 38.785 kΩ

The resonance impedance can be calculated from the digital output code as follows:

Equation 2.

Where:

Y=Proximity Data/2⁷

Rp_MAX and Rp_MIN are the maximum and minimum Rp values selected in the respective registers

Proximity data is the LDC output, register address 0x22.

Example: If Proximity data (address 0x22) is 50, Rp_MIN is 2.394 kΩ, and Rp_MAX is 38.785 kΩ, the resonance impedance is given by:

Y=50/2⁷ = 0.3906

Rp=(38785*2394)/(2394×(1-0.3906) + 38785×0.3906) =(92851290)/(15149.421 + 1458.9036)

Rp = 5.59 kΩ

7.4.1 Power Modes

The LDC1051 has two power modes:

• Active Mode : In this mode the Proximity data conversion is enabled.
• Stand-by Mode: This is the default mode on device power-up. In this mode conversion is disabled.

7.4.2 INTB terminal Modes

The INTB terminal is a configurable output terminal which can be used to drive an interrupt on an MCU. The LDC1051 provides three different modes on INTB terminal:

1. Comparator Mode
2. Wake-Up Mode
3. DRDY Mode

LDC1051 has built-in High and Low trigger threshold registers which can be used as a comparator with programmable hysteresis or in a special mode which can be used to wake-up an MCU. These modes are explained in detail below.

7.4.2.1 Comparator Mode

In the Comparator mode, the INTB terminal is asserted or deasserted when the proximity register value increases above Threshold High or decreases below Threshold Low registers respectively. In this mode, the LDC1051 essentially behaves as a proximity switch with programmable hysteresis.

Figure 11. Behavior Of INTB Terminal In Comparator Mode

7.4.2.2 Wake-Up Mode

In Wake-Up mode, the INTB terminal is asserted when proximity register value increases above Threshold High and de-asserted when wake-up mode is disabled in INTB terminal mode register.

This mode can be used to wake-up an MCU from sleep, to conserve power.

Figure 12. Behavior Of INTB Terminal In Wake-Up Mode

7.4.2.3 DRDYB Mode

In DRDY(Data Ready) mode, the INTB terminal is asserted every time the conversion data is available and de-asserted once the read command on register 0x22 is registered internally; if the read is in progress, the terminal is pulsed instead. The valid condition for new data availability is CSB high and DRDYB falling edge.

Figure 13. Behavior of INTB Terminal in DRDYB Mode with SPI Extending Beyond Subsequent Conversions

Figure 14. Behavior Of INTB Terminal In DRDYB Mode with SPI Reading The Data Within Subsequent Conversion

7.5.1 SPI Description

A typical serial interface transaction begins with an 8-bit instruction, which is comprised of a read/write bit (MSB, R=1) and a 7 bit address of the register, followed by a data field which is typically 8 bits. However, the data field can be extended to a multiple of 8 bits by providing sufficient SPI clocks. Refer to the Extended SPI Transactions section below.

Figure 15. Serial Interface Protocol

Each assertion of CSB starts a new register access. The R/Wb bit in the command field configures the direction of the access; a value of 0 indicates a write operation and a value of 1 indicates a read operation. All output data is driven on the falling edge of the serial clock (SCLK), and all input data is sampled on the rising edge of the serial clock (SCLK). Data is written into the register on the rising edge of the 16th clock. It is required to deassert CSB after the 16th clock; if CSB is deasserted before the 16th clock, no data write will occur.

Table 1. Register Map^(1)(2)(3)

Table 2. Revision ID

Table 3. Rp_MAX

Table 4. Register Settings for Rp_MAX

Table 5. Rp_MIN

Table 6. Register Settings for Rp_MIN

Table 7. Watchdog Timer Frequency

Address = 0x03, Default=0x45, Direction=R/W
Bit Field	Field Name	Description
7:0	Min Sensor Frequency	Sets the watchdog timer. The Watchdog timer is set based on the lowest sensor frequency. Equation 3. where F is the sensor frequency Example: If Sensor frequency is 1Mhz Min Sensor Frequency=68.94*log10(1M/2500)=Round to nearest integer(179.38)=179

Table 8. LDC Configuration

Table 9. Comparator Threshold High MSB

Table 10. Comparator Threshold Low MSB

Table 11. INTB Terminal Configuration

Table 12. Power Configuration

Table 13. Status

Table 14. Proximity Data