1. 1 Closed-Loop Modeling of Power and Temperature Profiles of FPGAs Kanupriya Gulati Sunil P. Khatri Peng Li Department of ECE, Texas A&M University, College Station

2. 2 Introduction Due to increasing density of FPGAs –Power is now a zeroth order design constraint During operation, two components of power consumption are –Dynamic Power Temperature independent –Static Power Gate leakage –Largely temperature independent Sub-threshold leakage –Exponential dependence on junction temperature This positive feedback loop could cause –Non-convergence (thermal runaway) –Convergence above a safe junction temperature (thermal breakdown) Increase in dynamic power Increase in temperature Increase in leakage power

3. 3 Our Approach Our approach is design and FPGA device specific Partition placed and routed FPGA design into n 2 grid regions For each grid region, at the given temperature –Compute total power (dynamic and leakage power) Dynamic power computed based on logic in the region Leakage power computed using fast and accurate macromodels From the power of the n 2 grid regions, compute new thermal profile –Compute increase in temperature for each grid region –If change in temperature in all grid regions is less than ε, stop and declare convergence –If no convergence and new temperature in any grid region more than a threshold value, declare thermal breakdown –Else recompute leakage power of each grid region using new temperature value and iterate

4. 4 Our Approach – Flowchart

5. 5 Our Approach – Dynamic Power Compute using the XPower tool from Xilinx –XPower reads the design data file and computes activity estimate ‘α’ –After synthesis, place and route of the design, we compute the maximum operating frequency ‘f ckt ’ –XPower has the node and wire capacitance values. So, P dyn = C * Vdd 2 * f ckt * α –Find the contribution of grid region (i, j) to P dyn For each LUT in grid region (i, j), we compute –Probability of output being logic ‘1’, P 1 = (ΣV k )/16 »Where V k is the logic value stored in the k th SRAM of the LUT –Probability of output switching, P sw = 2 * P 1 * (1-P 1 ) Average probability of switching in the grid region P(i, j) = (ΣP sw )/q –Where q is the number of LUTs per grid region P dyn (i, j) = P dyn * P(i, j) * 1/(ΣP(i, j))

6. 6 Our Approach – Static Power NMOS Passgate Gate Leakage States L 2 ’ Leakage NMOS Passgate Sub-threshold Leakage States LUT Implementation using a 16:1 MUX

7. 7 Our Approach – Static Power Pre-compute leakage using SPICE for –LUT SRAM configuration data is known Each of the 31 pass gates in LUT are in one of –4 states ( L 1, L 2, L 3 or L 2 ’ ) contributing to subthreshold leakage –4 states ( K 1, K 2, K 3 or K 4 ) contributing to gate leakage or –Remaining states have negligible leakage contribution But we do not know the f 1, f 2, f 3 and f 4 inputs to the LUT –Take average over 16 possible input combinations SRAM cell in LUT (stored 1 and 0) –D-flipflop (output 1 and 0) –MUX Logic block in the FPGA

8. 8 Our Approach – Total Power Generate temperature dependent leakage macromodel for –LUT ( L states), D-flipflop, SRAM and MUX Pre-compute the leakage values at 3 different temperatures and fit exponential curve Gate leakage (for K states) is largely temperature independent –Leakage is quickly and accurately estimated for the logic block at any temperature Maximum 3% error when compared to explicit SPICE runs 4 orders of magnitude faster Compute leakage for grid region ( i, j ) at any temperature, P lkg (i, j, T) –Taking the sum of the leakages of all LUTs, D-flipflops, SRAMs and MUXes in region ( i, j ) at any temperature T = temp(i, j) Total power P tot (i, j, T) = P dyn (i, j) + P lkg (i, j, T)

9. 9 Our Approach – Temperature Computation We use the following approach –“ Critical path analysis considering temperature, power supply variations and temperature induced leakage ”, P. Li, ISQED 2006 –Assume a 1W power consumption in grid region (i, j) Table Z ij (k, l) indicates resulting temperature at grid region (k, l) –We precompute n 2 such Z ij tables, each with n 2 entries –We know the total power consumption of each grid region Thus, we find the new temperature, temp_new(i,j), at the (i, j) th grid region, by superposition Details of the thermal model –Circuit discretized into n 2 grid regions –15 layers of metal/dielectric are modeled Assuming a metallization percentage for each layer, the thermal conductivity of each layer is computed –Model includes heat dissipation due to heat sinks

10. 10 Endgame and Experimental Setup Endgame –Find the absolute difference between temp(i,j) and temp_new(i,j) –Declare convergence when the maximum difference for all grid points is < 0.001°c –If temp_new(i,j) > 110°c, and no convergence, we declare thermal breakdown Setup –Applied our methodology to 10 designs, implemented on a Virtex-4XCVLX200 Xilinx FPGA device –Synthesized, placed and routed using Xilinx ISE 8.1 i –Initial temperature set at 27°c –n = 16 –To the best of our knowledge, no other existing work reports final converged temperature and power numbers for FPGA designs, after closing the dependence loop between leakage and temperature –We therefore compared our final temperatures against a full-chip 3D thermal modeling and simulation tool Maximum (average) error in temperature was 2.52%(1.05%) for the DMA benchmark Our approach is faster by ~40X per iteration

11. 11 Results Temperature Profile for Circuit DMA Circuits operating at 450 MHz

12. 12 Conclusions Developed a technique to simultaneously model (in an FPGA) –Power consumption –Temperature Used fast and accurate macromodels, for leakage estimation –Over all circuit components of a logic block, at all temperatures Less than 3% error compared to SPICE and Up to 4 orders of magnitude speedup Approach –Partition FPGA design (placed and routed) into 16x16 grid regions –Compute total power consumption (dynamic and leakage) for each region –Find thermal profile of IC under this power consumption Using pre-computed power-to-temperature tables –New thermal information is used to update the leakage power consumption –Steps iterated until the temperature converges (for all grid regions), or exceeds a safe value (for any grid region) Final temperature obtained from our method –Compared to full-chip 3D temperature estimation tool –Shows max.(avg.) error of 2.52%(1.05%) for the DMA benchmark