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Original Articles

Global time method for inverse heat conduction problem

, &
Pages 651-664 | Received 12 Feb 2012, Accepted 13 Feb 2012, Published online: 24 Apr 2012

Figures & data

Figure 1. Inverse results using N = 4 using errorless data: (a) temperature and (b) heat flux inverse predictions.

Figure 1. Inverse results using N = 4 using errorless data: (a) temperature and (b) heat flux inverse predictions.

Figure 2. Effect of the sampling rate on the inverse heat flux prediction with N = 7 using errorless data: (a) and (b) .

Figure 2. Effect of the sampling rate on the inverse heat flux prediction with N = 7 using errorless data: (a) and (b) .

Figure 3. Technique for estimating the noise present in the data: (a) first-order fit to data; (b) least-squares fit to residual; and (c) actual and estimated noises.

Figure 3. Technique for estimating the noise present in the data: (a) first-order fit to data; (b) least-squares fit to residual; and (c) actual and estimated noises.

Figure 4. Gaussian low-pass filter exploration: (a) optimum cut-off frequency range and (b) insensitivity of Gaussian filter to a small change in cut-off frequency.

Figure 4. Gaussian low-pass filter exploration: (a) optimum cut-off frequency range and (b) insensitivity of Gaussian filter to a small change in cut-off frequency.

Figure 5. Inverse results using a normal distribution, with a standard deviation of 0.01 and a dimensionless cut-off frequency of 2.6: (a) noisy data used as input to the inverse code; (b) inverse temperature results and (c) inverse heat flux results.

Figure 5. Inverse results using a normal distribution, with a standard deviation of 0.01 and a dimensionless cut-off frequency of 2.6: (a) noisy data used as input to the inverse code; (b) inverse temperature results and (c) inverse heat flux results.

Figure 6. Temperature data for Beck triangle problem: (a) raw data with σ = 0.01 and (b) insensitivity of Gaussian filter to change in cut-off frequency.

Figure 6. Temperature data for Beck triangle problem: (a) raw data with σ = 0.01 and (b) insensitivity of Gaussian filter to change in cut-off frequency.

Figure 7. Inverse results for the classical Beck triangle problem for: (a) surface temperature prediction and (b) surface heat flux prediction. Noise was simulated using a normal distribution, σ = 0.01 and used for regularization.

Figure 7. Inverse results for the classical Beck triangle problem for: (a) surface temperature prediction and (b) surface heat flux prediction. Noise was simulated using a normal distribution, σ = 0.01 and used for regularization.

Table 1. Predicted heat flux RMS error as a function of the sampling rate, , projection order, N and choice of cut-off frequency, and qRMS,mean are average values resulting from five independent noise distributions.

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