Recall the essence of data transmission: How Computers Work Lecture 11
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1 Recall the essence of data transmission: How Computers Work Lecture 11 Q: What form does information take during transmission? Introduction to the Physics of Computation A: Energy Energy How Computers Work Lecture 11 Page 1 How Computers Work Lecture 11 Page 2 1
2 Recall the SR Flop in the Store State H Is this an adequate way to explain storage of a bit? A: No No Vin Vout Vout Vout > Vin Vout = Vin H Vout < Vin Vin How Computers Work Lecture 11 Page 3 How Computers Work Lecture 11 Page 4 2
3 Where is the bit really stored? In In the the capacitors capacitors A little exercise: In a world of Rs, Ls, Cs, and Memory-less gain elements, only the Ls Ls and Cs Cs store energy, so memory can only reside in them. These elements inevitably cause delay. Memory Requires Delay Delay Delay, Energy, and State (Memory) are intimately coupled. How Computers Work Lecture 11 Page 5 How Computers Work Lecture 11 Page 6 3
4 (Linear) Capacitor Energetics Q: How much energy does a capacitor charged to voltage V store? (1/2) A: (1/2) C V2 V 2 Q: If I charge an originally discharged capacitor to a voltage V through a resistor, how much energy is dissipated in the resistor? A: (1/2) (1/2) C V2 V 2 Q: How much total energy is lost charging (to V) and discharging a capacitor? C V2 A: C V 2 V R C Power Loss in the CMOS Inverter Power is lost due to: 1) Leakage Leakage Shoot-Through 2) Shoot-Through 3) Capacitive Capacitive Charge/Discharge Charge/Discharge In Q How Computers Work Lecture 11 Page 7 How Computers Work Lecture 11 Page 8 4
5 Quantitative Power Loss in CMOS Leakage: Insignificant Insignificant Crossover (Shoot-Through): Small if Rise/Fall times are fast Small if Rise/Fall times are fast Capacitive: Constant Energy / Cycle, ergo: Power is proportional to Frequency Power is proportional to How do we minimize power loss? G S D Q: Does changing the on-resistance help? A: No Q: Does making the channel length shorter help? A: Yes - C Q: Does lowering the voltage help?a: Yes Yes No Yes - C goes goes down down How Computers Work Lecture 11 Page 9 How Computers Work Lecture 11 Page 10 5
6 But do MOS transistors turn on enough at low voltages? How about speed? V R S Side View G A: Yes Yes as long as you doctor the channel a bit, thus lowering the turn-on threshold. D In Q Unlike power dissipation, lowering R does lower Tpd. Q: How do we lower R? Shorter A: Make FET channel Shorter Q: Does making the FET channel wider help? A: No No because it raises C while lowering R. S Side View Top View G D C How Computers Work Lecture 11 Page 11 How Computers Work Lecture 11 Page 12 6
7 What about the gate oxide thickness? Q: If it takes a fixed E-field strength to turn on the transistor, what effect does changing the gate oxide thickness have? A: An n times thicker gate oxide takes roughly n n times more voltage to make the same E-field strength, but has roughly 1/n 1/n times the capacitance as before. Thus, thicker oxides are a net. loss loss Ergo: Gate oxides are made as thin thin as possible, given reliability constraints. Other ways of lowering power consumption: Re-Code data for fewer transitions. Re-design architectures for fewer transition in average case performance. Power-Down (i.e. selectively clock) parts of a machine that aren t needed now. Consider radical ideas like reversible computing. How Computers Work Lecture 11 Page 13 How Computers Work Lecture 11 Page 14 7
8 Reversible Computing? The smallest energy system we know that can represent a bit: Q1: How little energy can be used to represent a bit? Q2: Is there a minimum energy is takes to do computation? Intuitive (in this case, wrong) answers: A1: It can take arbitrarily little energy to represent a bit A2: Computation must consume power Heat Source/Sink at T 1 particle of gas exists in a 2-piston iso-thermal cylinder at temperature T. Q: What is the kinetic energy of the particle? How Computers Work Lecture 11 Page 15 A: T T How Computers Work Lecture 11 Page 16 8
9 Q: Does it take energy to slowly compress the gas to the left side? Then why did it take energy? A: Yes Yes Q: Is the kinetic energy of the particle any different? A: No No Heat Source/Sink at T How Computers Work Lecture 11 Page 17 Heat Source/Sink at T A: Because the particle was bouncing against the piston Q: Where did this energy go? A1: Into the heat sink A2: Into information! How Computers Work Lecture 11 Page 18 9
10 How many bits of information have we created? Can we get this energy back? 1 A: 1 Q: How much energy did this take: Heat Source/Sink at T Yes A:!!!!!! Yes IF WE DO IT SLOWLY!!!!! Heat Source/Sink at T A: log e (2) k T How Computers Work Lecture 11 Page 19 How Computers Work Lecture 11 Page 20 10
11 Summary: Slow (i.e. reversible) thermodynamic processes can recover the energy put into creating a bit. Fast (i.e. irreversible) processes loose part of this energy. We can recover an arbitrarily high fraction of the energy put in by going slowly enough. There s nothing special about the isothermal heat sink - adiabatic (insulated) cylinders work too, it s the speed that s important. But that s bit storage. How about computing? A: Computing is nothing more than creating bits whose value is determined by examining other bits. Examination of bits is energetically free. It is their creation and destruction that is tied to energy. When destroying a bit, we can do so reversibly (i.e. slowly) or irreversibly (i.e. fast). How Computers Work Lecture 11 Page 21 How Computers Work Lecture 11 Page 22 11
12 A typical CMOS Inverter But there s another way: Has fixed power supply rails. Is driven as fast as possible. Operates non-reversibly. Throws away its bit energy In Q Reversible Computing: To Create a bit: Start with two power supply rails at the same voltage. Connect the parasitic capacitance to the appropriate power supply rail. Slowly separate the power supply rail voltages, raising one and lowering the other. To (reversibly) destroy a bit: Start with two power supply rails separated by some voltage. Connect the (already charged) parasitic capacitance to the appropriate rail. Slowly bring the power supply rails together. Except for (arbitrarily small) resistive losses, the power supply can recover all of the energy! How Computers Work Lecture 11 Page 23 How Computers Work Lecture 11 Page 24 12
13 An example: Younis and Knight s SCRL = Clock Lines Out An interesting consequence: We must remember the value of a bit in order to recover it s energy, so every computation must be reversed after it is done. Thus: For any computation (e.g. AND) that destroys input information, we must remember enough input variables to be able to UNDO or REVERSE the computation, and recover the energy that would be otherwise lost due to the DESTRUCTION OF BITS. In This is sometimes practical and sometimes not. By being clever and only throwing away bits when it is very inconvenient to remember them, we can make reversible computation practical. How Computers Work Lecture 11 Page 25 How Computers Work Lecture 11 Page 26 13
14 Reversible Computing? Some real answers Q1: How little energy can be used to represent a bit? Q2: Is there a minimum energy is takes to do computation? Real answers: A1: k T log e (2) is the minimum energy to reliably store a bit CMOS gates typically use 10 8 kt per bit RNA duplication typically uses 100 kt per bit To Learn More Read: Feynman Lectures on Computation Thermodynamics of Computation - A Review Charles H. Bennett, International Journal of Theoretical Physics 21, 905(1982) A2: Computation does NOT need to consume power, as long as it is done reversibly (i.e. slowly enough, and without destroying information) Related Trivia : The awake human brain consumes approximately 40 Watts of power. How Computers Work Lecture 11 Page 27 How Computers Work Lecture 11 Page 28 14
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