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Thermodynamic Perspective on Architectures

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Thermodynamic Perspective on Architectures Sadasivan Shankar (Intel) Ack: Ralph K. Cavin III (SRC), Victor V. Zhirnov (SRC) July 12 Emerging Research on Architectures – PowerPoint PPT presentation

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Title: Thermodynamic Perspective on Architectures


1
Thermodynamic Perspective on Architectures
  • Sadasivan Shankar (Intel)
  • Ack Ralph K. Cavin III (SRC), Victor V. Zhirnov
    (SRC)
  • July 12
  • Emerging Research on Architectures
  • ERD Meeting, San Francisco

2
Main Points
  • We have developed a general methodology for
    applying thermodynamic principles for information
    engines like the Carnot principle to heat engines
  • More fundamental than simplistic capacitance
    based formalism currently being used
  • The operating limit of 104 kT is possibly due to
    quantum state, architecture, and layout
  • Two applications
  • Similar to heat engines, will identify the ideal
    Compute Engine Carnots Compute Engine for
    ideal computing. This would serve as a limiting
    case for realistic architectures
  • Estimate efficiencies for different architectures
    based on physics
  • Layout efficiency
  • Energy efficiency
  • Potential trade-off between layout and energy
  • Continue work on estimating minimum energy needed
    of various simple systems

3
Computing Engine Premise
Heat Engine
Computing Engine
  • Similar to a heat engine, a computing engine can
    be visualized
  • Goal is to use thermodynamics, which incorporates
    relations between systems components and
    determines the most energy efficient systems

4
A Perspective on Layout
  • Ideal layout based on a single switch
  • Interconnects and isolation may be driving in
    real systems

5
Entropy of a Single Switch System (1)
  • Entropy is determined by statistical mechanics

Switching state
Quantum States
Nit Nit 2 is bit, Nit 4 is qit etc. kB -
Boltzmann constant N number of states in the
system (1 for single state switching) Et Total
Energy is estimated from statistical mechanics Z
Partition function
Switching Energy
Total energy
6
Free Energy of a Single Switch System
  • Free energy is determined by thermodynamics

7
Simple Illustration
  • For a binary switch, the minimum energy is
    determined by the need to maintain binary
    transition (bit) and energy of the particle in an
    isolated level
  • For a classical switch, the following are the
    limits

Example Micro-Systems Bits N Pi EMin
Binary 1 D2/8a2 1/2N kT log 2
Inverter 1 D2/12a2 1/2N kT log 2
NOR 2 D2/24a2 1/4N 2kT log 2
NAND 2 D2/16a2 1/4N 2kT log 2
6-T SRAM 16 D2/48a2 1/216N 16kT log 2
  • EMin is idealistic and is determined by the bits
    processed in the micro-systems

8
Ideal Architecture Comparison A Simple
Illustration
U 4 (14 x 10) Nit 16, 16, 16,16
U 8 (10 x 12) Nit 2, 2, 2, 2
  • For an ideal classic switch, reducing minimum
    energy seems to be driven by U more than Nit (due
    to log Nit dependence)
  • Indicates that fewer larger units with larger
    bits processed in each lower free energy for a
    classical switch
  • Other factors not considered
  • Interconnects, dissipation, functionality of
    architecture, unit layout, software, .
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