Johnson Ring Counter

#shift registers #johnson ring counter #circuit design #timing diagram #frequency division #sequential logic #pattern generation #digital circuits #logic design

1. Definition and Basic Concept

Johnson Ring Counter: Definition and Basic Concept

A Johnson ring counter, also known as a twisted ring counter or Möbius counter, is a synchronous shift register with the inverted output of the last stage fed back into the input of the first stage. This feedback mechanism creates a circulating pattern of bits that distinguishes it from conventional ring counters.

Mathematical Foundation

The state sequence of an n-stage Johnson counter follows a predictable cyclic pattern with a modulus of 2n, double that of a standard ring counter. The state transitions can be described by:

$$ Q_{i}^{t+1} = \begin{cases} \overline{Q_{n-1}^{t}} & \text{for } i = 0 \\ Q_{i-1}^{t} & \text{for } 1 \leq i \leq n-1 \end{cases} $$

where Qit represents the state of the i-th flip-flop at time t.

Circuit Architecture

The canonical implementation consists of:

Characteristic Waveforms

The output generates a quadrature phase relationship between stages, making it valuable for:

Key Advantages Over Standard Counters

Feature Johnson Counter Binary Counter
State Decoding Requires only 2-input AND gates Needs full decoder
Glitch Immunity Single-bit changes between states Multiple bits may change
Power Consumption Lower dynamic power Higher switching activity

Historical Context

First patented by Robert Royce Johnson in 1953 while at Sperry Gyroscope Company, the design emerged as a solution for reliable position encoding in early electromechanical navigation systems. Its inherent fault tolerance made it particularly valuable in aerospace applications.

Definition and Basic Concept in Johnson Ring Counter
Diagram Description: The feedback mechanism and quadrature phase relationships are highly visual concepts that require spatial representation.

1.2 Working Principle

The Johnson Ring Counter, also known as a twisted ring counter, is a synchronous shift register with feedback that generates a cyclic sequence of states. Unlike a standard ring counter, where the output of the last flip-flop feeds directly back to the input of the first, the Johnson counter inverts the feedback signal, resulting in a sequence length of 2N for an N-stage counter.

State Transition Mechanism

The counter operates by propagating a single high or low bit through a series of D-type flip-flops, with the complement of the final output fed back to the input. For a 4-stage Johnson counter (N=4), the sequence proceeds as follows:

$$ Q_0 Q_1 Q_2 Q_3 \rightarrow \overline{Q_3} Q_0 Q_1 Q_2 $$

Each clock pulse shifts the existing bits right and inserts the inverted last bit at the first stage. The complete 8-state sequence for a 4-stage counter is:

  1. 0000 → 1000
  2. 1000 → 1100
  3. 1100 → 1110
  4. 1110 → 1111
  5. 1111 → 0111
  6. 0111 → 0011
  7. 0011 → 0001
  8. 0001 → 0000 (cycle repeats)

Mathematical Basis

The state transitions follow Boolean logic, where for an N-bit counter, the next state Sn+1 is derived from the current state Sn as:

$$ S_{n+1} = (S_n \gg 1) \, | \, ((\sim S_n \,\&\, 1) \ll (N-1)) $$

where ≫ denotes a right shift, | is bitwise OR, ∼ is inversion, and ≪ is a left shift. The modulus of the sequence is always 2N, providing higher state density than a standard ring counter (modulus N).

Timing and Synchronization

Since the Johnson counter is synchronous, all flip-flops update on the rising or falling edge of a shared clock signal. The propagation delay tpd must satisfy:

$$ t_{pd} < T_{clock} - t_{setup} $$

where Tclock is the clock period and tsetup is the flip-flop setup time. Metastability can occur if this constraint is violated.

Applications

D0 D1 D2 CLK
Working Principle in Johnson Ring Counter
Diagram Description: The diagram would physically show the feedback path and clock connections between flip-flops, illustrating the inversion mechanism that distinguishes a Johnson counter from a standard ring counter.

1.3 Comparison with Other Shift Registers

The Johnson ring counter, while functionally similar to other shift registers, exhibits distinct differences in operation, efficiency, and application. Below, we compare it with three common shift register types: the serial-in serial-out (SISO), parallel-in parallel-out (PIPO), and the standard ring counter.

Serial-In Serial-Out (SISO) Shift Register

A SISO shift register processes data sequentially, with each bit shifted through the register one at a time. The Johnson counter, in contrast, recycles its output back to the input, creating a closed loop. While a SISO requires N clock cycles to load N bits, a Johnson counter with N flip-flops produces 2N distinct states, doubling its effective state space. This makes the Johnson counter more efficient for applications requiring repetitive pattern generation, such as in LED chasers or frequency dividers.

Parallel-In Parallel-Out (PIPO) Shift Register

PIPO registers allow simultaneous loading and reading of all bits, making them ideal for high-speed data transfer. However, they lack the Johnson counter's inherent state sequencing capability. The Johnson counter's ability to generate a continuous, non-repeating sequence of states (until all 2N states are exhausted) is advantageous in control systems where deterministic state transitions are critical, such as in stepper motor controllers.

Standard Ring Counter

A standard ring counter circulates a single '1' or '0' through its flip-flops, producing only N unique states for N flip-flops. The Johnson counter's modified feedback mechanism (inverting the output before feeding it back) doubles the number of states to 2N. This property is mathematically expressed as:

$$ S_{Johnson} = 2N $$

where SJohnson is the number of unique states. The standard ring counter's state count remains:

$$ S_{Ring} = N $$

Power and Area Efficiency

Johnson counters typically consume less power than PIPO registers due to reduced parallel data switching. However, they require more flip-flops than a SISO for equivalent state coverage. For example, a 4-bit Johnson counter (8 states) needs 4 flip-flops, while a 3-bit SISO (8 states) requires only 3. The trade-off between state density and hardware complexity must be evaluated based on application constraints.

Applications in Digital Systems

2. Components Required

2.1 Components Required

A Johnson Ring Counter, also known as a twisted ring counter, is a sequential logic circuit constructed using a shift register with an inverted feedback loop. The following components are essential for its implementation:

Primary Components

Supporting Components

Optional Enhancements

Component Selection Criteria

Critical parameters for flip-flop selection include:

$$ t_{su} < T_{clock} - t_{prop,feedback} $$

where tsu is the flip-flop setup time and tprop,feedback is the cumulative propagation delay through the feedback path. For CMOS implementations, ensure:

$$ f_{max} = \frac{1}{N \times (t_{PHL} + t_{PLH})} $$

where N is the number of stages and tPHL/tPLH are output transition times.

Practical Implementation Notes

For a 4-stage Johnson counter (8 unique states), the component count would be:

2.2 Circuit Diagram and Explanation

The Johnson ring counter, also known as a twisted ring counter, is a synchronous shift register with feedback from the inverted output of the last stage to the input of the first stage. This configuration generates a sequence of states that cycles through 2N unique patterns for an N-stage counter, unlike a standard ring counter which only produces N states.

Circuit Topology

The basic Johnson counter consists of:

D FF1 D FF2 D FF3 CLK

State Transition Analysis

The counter progresses through states according to the following rules:

$$ Q_{n}^{t+1} = Q_{n-1}^t \quad \text{for } n > 1 $$ $$ Q_{1}^{t+1} = \overline{Q_N}^t $$

For a 4-stage counter, the complete state sequence is:

Clock Pulse Q1 Q2 Q3 Q4
0 0 0 0 0
1 1 0 0 0
2 1 1 0 0
3 1 1 1 0
4 1 1 1 1
5 0 1 1 1
6 0 0 1 1
7 0 0 0 1
8 0 0 0 0

Timing Considerations

The maximum operating frequency is determined by:

$$ f_{max} = \frac{1}{t_{pd(FF)} + t_{pd(INV)} + t_{su}} $$

where tpd(FF) is flip-flop propagation delay, tpd(INV) is inverter delay, and tsu is setup time. Metastability can occur if these timing constraints are violated during the feedback loop.

Practical Implementation Notes

Johnson Ring Counter Circuit Topology Schematic diagram showing the interconnection of D flip-flops with feedback through an inverter and clock distribution in a Johnson Ring Counter. D FF1 Q Q̅ D FF2 Q Q̅ D FF3 Q Q̅ Feedback Inverter CLK
Diagram Description: The diagram would physically show the interconnection of D flip-flops with feedback through an inverter and clock distribution.

2.3 Timing Diagram Analysis

Clock Synchronization and State Transition

The Johnson Ring Counter operates synchronously, with state transitions occurring at the rising or falling edge of the clock signal. For an n-stage counter, the timing diagram illustrates how each flip-flop (FF0 to FFn-1) propagates its output after a clock edge. The propagation delay (tpd) between stages must satisfy:

$$ t_{pd} < T_{clk} - t_{setup} $$

where Tclk is the clock period and tsetup is the setup time of the flip-flops. Violating this condition leads to metastability or incorrect state transitions.

Waveform Interpretation

The timing diagram for a 4-stage Johnson counter (8 unique states) shows:

CLK Q₀ Q₁

Critical Timing Parameters

The following parameters govern correct operation:

$$ f_{max} = \frac{1}{n \cdot t_{pd} + t_{setup}} $$

Practical Implications

In high-speed applications (e.g., serial-to-parallel converters), timing mismatches introduce jitter. SPICE simulations or hardware logic analyzers are used to validate the timing diagram against theoretical predictions. For fault tolerance, designers often include:

Timing Diagram Analysis in Johnson Ring Counter
Diagram Description: The timing diagram physically shows the clock signal and corresponding output waveforms (Q₀ to Q₃) with their phase relationships and propagation delays.

3. Frequency Division

3.1 Frequency Division

A Johnson Ring Counter inherently performs frequency division due to its circulating shift-register structure. For an n-stage counter, the output frequency at any given stage is 1/(2n) of the input clock frequency. This property arises because the counter requires 2n clock cycles to complete one full cycle of its state sequence.

Mathematical Derivation

Consider an n-bit Johnson counter. The total number of unique states is 2n, as each bit propagates through the shift register and inverts upon completing the loop. The output frequency fout is derived as follows:

$$ f_{out} = \frac{f_{clk}}{2n} $$

where:

Practical Implications

This frequency division is useful in applications requiring subharmonic clock generation, such as:

Phase-Shifted Outputs

Each stage of the Johnson counter provides a signal with a phase shift of 360°/(2n) relative to the previous stage. For example, a 4-stage counter (n=4) yields outputs with 45° phase separation, useful in polyphase signal generation.

$$ \Delta\phi = \frac{360°}{2n} $$

Stability and Noise Considerations

Unlike binary counters, Johnson counters exhibit reduced glitch-related noise during state transitions, as only one bit changes at a time. This makes them advantageous in high-precision frequency division where spurious transitions must be minimized.

Real-World Example

In a 5-stage Johnson counter (n=5), a 10 MHz clock input produces a 1 MHz output (fout = 10 MHz / (2×5) = 1 MHz). This is commonly used in decade counter applications where a clean, glitch-free division-by-10 is required.

Frequency Division in Johnson Ring Counter
Diagram Description: The diagram would show the phase-shifted outputs and frequency division relationship across stages of the Johnson counter.

3.2 Pattern Generation

Fundamentals of Pattern Sequencing

A Johnson ring counter, also known as a twisted ring counter, generates a deterministic sequence of states by feeding the inverted output of the last flip-flop back to the input of the first. For an n-stage counter, this produces 2n unique states, unlike a standard ring counter’s n states. The pattern evolves as a walking ring of alternating 1s and 0s, with a Hamming distance of 1 between consecutive states.

$$ Q_{i}(t+1) = \overline{Q_{n-1}(t)} \quad \text{(for } i=0\text{)} $$ $$ Q_{i}(t+1) = Q_{i-1}(t) \quad \text{(for } 1 \leq i \leq n-1\text{)} $$

State Transition Analysis

Consider a 4-bit Johnson counter initialized to 0000. The sequence progresses as follows:

Clock Cycle 0: 0000 1: 1000 2: 1100 3: 1110

After reaching 1111, the sequence mirrors backward (0111 → 0011 → ...), forming a closed loop. The state transition graph is a Hamiltonian cycle through all possible 2n configurations.

Applications in Control Systems

Johnson counters are favored in:

Case Study: Stepper Motor Control

A 4-bit Johnson counter driving an H-bridge produces the sequence 1000 → 1100 → 0100 → 0110 → ..., enabling full-step control of a bipolar stepper motor with minimal glitch power dissipation.

Mathematical Derivation of Sequence Length

The number of unique states L for an n-stage counter is derived from the recurrence relation:

$$ L(n) = 2n $$

This contrasts with a linear feedback shift register (LFSR), where L = 2n − 1. The reduced state space simplifies decoding logic in applications like rotary switch debouncing.

Pattern Generation in Johnson Ring Counter
Diagram Description: A state transition diagram would physically show the Hamiltonian cycle of the 4-bit Johnson counter's sequence from 0000 to 1111 and back.

Johnson Ring Counter

Structure and Operation

A Johnson ring counter, also known as a twisted ring counter, is a modified shift register where the inverted output of the last stage is fed back to the input of the first stage. This feedback mechanism creates a unique sequence of states that cycles through 2N distinct patterns for an N-stage counter, unlike a standard ring counter which cycles through only N states.

The basic structure consists of D-type flip-flops connected in series, with the Q' (complementary output) of the final stage driving the D input of the first stage. For a 4-stage Johnson counter, the state transition sequence is:

$$ 0000 \rightarrow 1000 \rightarrow 1100 \rightarrow 1110 \rightarrow 1111 \rightarrow 0111 \rightarrow 0011 \rightarrow 0001 \rightarrow 0000 $$

Mathematical Analysis

The maximum count length L of an N-bit Johnson counter is given by:

$$ L = 2N $$

Propagation delay (tp) is critical for high-speed operation. For a cascade of N flip-flops with individual delay tff:

$$ t_p = N \cdot t_{ff} $$

Applications

Design Considerations

To initialize the counter, a reset circuit forces all flip-flops to a known state (typically all zeros). Metastability risks arise if the feedback loop violates setup/hold times, necessitating:

$$ t_{clk} > N \cdot t_{ff} + t_{setup} $$

where tclk is the clock period and tsetup is the flip-flop setup time.

Power Consumption

Dynamic power dissipation scales quadratically with clock frequency (f) due to capacitive charging:

$$ P_{dynamic} = C_{eff} V_{DD}^2 f $$

where Ceff is the effective switched capacitance per stage.

Sequential Logic Circuits in Johnson Ring Counter
Diagram Description: The diagram would physically show the feedback connection between flip-flops and the state transition sequence.

4. Key Benefits

4.1 Key Benefits

High Noise Immunity and Robustness

The Johnson Ring Counter exhibits superior noise immunity compared to standard binary counters due to its use of a closed-loop shift register. Since only one bit changes state at a time (unlike binary counters where multiple bits may toggle simultaneously), the counter is less susceptible to transient noise and glitches. This makes it ideal for high-reliability applications such as industrial automation and aerospace systems.

Simplified Decoding Logic

A Johnson counter with n flip-flops produces 2n distinct states, allowing straightforward decoding without complex combinational logic. The output sequence follows a predictable pattern (e.g., 0000 → 1000 → 1100 → 1110 → 1111 → 0111 → 0011 → 0001 → 0000), enabling efficient state detection using minimal AND gates. This reduces propagation delays and power consumption in finite-state machine designs.

$$ \text{Number of states} = 2n $$

Self-Correcting Property

Unlike conventional ring counters, the Johnson configuration inherently corrects invalid states due to its feedback mechanism. If the counter enters an erroneous state (e.g., from a power glitch), it automatically returns to a valid state within n clock cycles. This eliminates the need for external reset circuitry in mission-critical systems.

Low Power Consumption

The single-bit transition property minimizes dynamic power dissipation, governed by:

$$ P_{dynamic} = \alpha C V^2 f $$

where α (activity factor) is significantly lower than in binary counters. This advantage is critical for battery-operated and IoT devices.

Phase Generation and Clock Division

The Johnson counter naturally generates 2n non-overlapping phases, useful in multi-phase clock systems. For example, a 4-stage counter divides the input clock by 8 while providing eight 45°-spaced phases, simplifying quadrature modulation/demodulation in RF systems.

Applications in High-Speed Systems

The absence of combinational logic between stages allows operation at higher frequencies than synchronous binary counters. This is exploited in:

Key Benefits in Johnson Ring Counter
Diagram Description: The diagram would show the closed-loop shift register configuration and the sequence of state transitions (e.g., 0000 → 1000 → 1100 → etc.) to visually demonstrate the counter's operation and self-correcting property.

4.2 Common Challenges and Solutions

Race Conditions and Timing Hazards

Johnson ring counters rely on synchronous clocking to ensure proper state transitions. However, propagation delays in flip-flops can lead to race conditions, where intermediate states are incorrectly sampled. The worst-case scenario occurs when the delay between stages (tpd) approaches half the clock period (Tclk/2). To mitigate this:

$$ t_{pd(max)} < \frac{T_{clk}}{2} - t_{setup} $$

Where tsetup is the setup time of the flip-flops. For high-frequency operation, use edge-triggered flip-flops with low propagation delay (e.g., 74HC74 for TTL logic).

Power-On Reset (POR) Issues

Without a reset mechanism, the counter may initialize to an invalid state (e.g., 0101). Solutions include:

Glitches in Decoding Logic

When deriving outputs from intermediate flip-flop states, combinatorial logic may produce transient glitches. For a 4-stage counter, the hazard-free decoding equation for state Sn is:

$$ S_n = Q_n \cdot \overline{Q_{n+1}} $$

Implement this with 2-input AND gates where one input is inverted. For higher noise immunity, add Schmitt triggers or pipeline the outputs.

Clock Skew Management

Uneven clock distribution causes stage-to-stage skew, degrading maximum operating frequency. To minimize skew:

Metastability in Feedback Path

The inverted feedback from the last stage creates a potential metastability point. The probability of metastability (Pmeta) is:

$$ P_{meta} = e^{-\frac{t_r}{\tau}} $$

Where tr is the reset time constant and τ is the flip-flop's metastability resolution time. Use flip-flops with built-in metastability hardening (e.g., 74FXX series) for critical applications.

EMI and Power Supply Noise

High-speed toggling generates broadband EMI. Countermeasures include:

Thermal Effects on Propagation Delay

For every 10°C rise in temperature, CMOS propagation delay increases by ~3%. In precision timing applications:

Common Challenges and Solutions in Johnson Ring Counter
Diagram Description: The section discusses race conditions and timing hazards, which are best visualized with clock period and propagation delay relationships.

5. Recommended Books

5.1 Recommended Books

5.2 Research Papers and Articles

5.3 Online Resources