예제 #1
0
파일: customfield.go 프로젝트: jsampaio/3
// mul1N pointwise multiplies a scalar (1-component) with an N-component vector,
// yielding an N-component vector stored in dst.
func mul1N(dst, a, b *data.Slice) {
	util.Assert(a.NComp() == 1)
	util.Assert(dst.NComp() == b.NComp())
	for c := 0; c < dst.NComp(); c++ {
		cuda.Mul(dst.Comp(c), a, b.Comp(c))
	}
}
예제 #2
0
파일: customfield.go 프로젝트: jsampaio/3
func divN1(dst, a, b *data.Slice) {
	util.Assert(dst.NComp() == a.NComp())
	util.Assert(b.NComp() == 1)
	for c := 0; c < dst.NComp(); c++ {
		cuda.Div(dst.Comp(c), a.Comp(c), b)
	}
}
예제 #3
0
파일: madd.go 프로젝트: jsampaio/3
// multiply-add: dst[i] = src1[i] * factor1 + src2[i] * factor2 + src3 * factor3
func Madd3(dst, src1, src2, src3 *data.Slice, factor1, factor2, factor3 float32) {
	N := dst.Len()
	nComp := dst.NComp()
	util.Assert(src1.Len() == N && src2.Len() == N && src3.Len() == N)
	util.Assert(src1.NComp() == nComp && src2.NComp() == nComp && src3.NComp() == nComp)
	cfg := make1DConf(N)
	for c := 0; c < nComp; c++ {
		k_madd3_async(dst.DevPtr(c), src1.DevPtr(c), factor1,
			src2.DevPtr(c), factor2, src3.DevPtr(c), factor3, N, cfg)
	}
}
예제 #4
0
파일: resize.go 프로젝트: callistoaz/3
// Select and resize one layer for interactive output
func Resize(dst, src *data.Slice, layer int) {
	dstsize := dst.Size()
	srcsize := src.Size()
	util.Assert(dstsize[Z] == 1)
	util.Assert(dst.NComp() == 1 && src.NComp() == 1)

	scalex := srcsize[X] / dstsize[X]
	scaley := srcsize[Y] / dstsize[Y]
	util.Assert(scalex > 0 && scaley > 0)

	cfg := make3DConf(dstsize)

	k_resize_async(dst.DevPtr(0), dstsize[X], dstsize[Y], dstsize[Z],
		src.DevPtr(0), srcsize[X], srcsize[Y], srcsize[Z], layer, scalex, scaley, cfg)
}
예제 #5
0
파일: shift.go 프로젝트: kyeongdong/3
// shift dst by shx cells (positive or negative) along X-axis.
// new edge value is clampL at left edge or clampR at right edge.
func ShiftX(dst, src *data.Slice, shiftX int, clampL, clampR float32) {
	util.Argument(dst.NComp() == 1 && src.NComp() == 1)
	util.Assert(dst.Len() == src.Len())
	N := dst.Size()
	cfg := make3DConf(N)
	k_shiftx_async(dst.DevPtr(0), src.DevPtr(0), N[X], N[Y], N[Z], shiftX, clampL, clampR, cfg)
}
예제 #6
0
파일: madd.go 프로젝트: jsampaio/3
// multiply: dst[i] = a[i] * b[i]
// a and b must have the same number of components
func Mul(dst, a, b *data.Slice) {
	N := dst.Len()
	nComp := dst.NComp()
	util.Assert(a.Len() == N && a.NComp() == nComp && b.Len() == N && b.NComp() == nComp)
	cfg := make1DConf(N)
	for c := 0; c < nComp; c++ {
		k_mul_async(dst.DevPtr(c), a.DevPtr(c), b.DevPtr(c), N, cfg)
	}
}
예제 #7
0
파일: conv_copypad.go 프로젝트: jsampaio/3
// Copies src into dst, which is larger, and multiplies by vol*Bsat.
// The remainder of dst is not filled with zeros.
// Used to zero-pad magnetization before convolution and in the meanwhile multiply m by its length.
func copyPadMul(dst, src, vol *data.Slice, dstsize, srcsize [3]int, Msat MSlice) {
	util.Argument(dst.NComp() == 1 && src.NComp() == 1)
	util.Assert(dst.Len() == prod(dstsize) && src.Len() == prod(srcsize))

	cfg := make3DConf(srcsize)

	k_copypadmul2_async(dst.DevPtr(0), dstsize[X], dstsize[Y], dstsize[Z],
		src.DevPtr(0), srcsize[X], srcsize[Y], srcsize[Z],
		Msat.DevPtr(0), Msat.Mul(0), vol.DevPtr(0), cfg)
}
예제 #8
0
// Copies src into dst, which is larger, and multiplies by vol*Bsat.
// The remainder of dst is not filled with zeros.
// Used to zero-pad magnetization before convolution and in the meanwhile multiply m by its length.
func copyPadMul(dst, src, vol *data.Slice, dstsize, srcsize [3]int, Bsat LUTPtr, regions *Bytes) {
	util.Argument(dst.NComp() == 1 && src.NComp() == 1)
	util.Assert(dst.Len() == prod(dstsize) && src.Len() == prod(srcsize))

	cfg := make3DConf(srcsize)

	k_copypadmul_async(dst.DevPtr(0), dstsize[X], dstsize[Y], dstsize[Z],
		src.DevPtr(0), vol.DevPtr(0), srcsize[X], srcsize[Y], srcsize[Z],
		unsafe.Pointer(Bsat), regions.Ptr, cfg)
}
예제 #9
0
파일: heun.go 프로젝트: kyeongdong/3
// Adaptive Heun method, can be used as solver.Step
func (_ *Heun) Step() {
	y := M.Buffer()
	dy0 := cuda.Buffer(VECTOR, y.Size())
	defer cuda.Recycle(dy0)

	if FixDt != 0 {
		Dt_si = FixDt
	}

	dt := float32(Dt_si * GammaLL)
	util.Assert(dt > 0)

	// stage 1
	torqueFn(dy0)
	cuda.Madd2(y, y, dy0, 1, dt) // y = y + dt * dy

	// stage 2
	dy := cuda.Buffer(3, y.Size())
	defer cuda.Recycle(dy)
	Time += Dt_si
	torqueFn(dy)

	err := cuda.MaxVecDiff(dy0, dy) * float64(dt)

	// adjust next time step
	if err < MaxErr || Dt_si <= MinDt || FixDt != 0 { // mindt check to avoid infinite loop
		// step OK
		cuda.Madd3(y, y, dy, dy0, 1, 0.5*dt, -0.5*dt)
		M.normalize()
		NSteps++
		adaptDt(math.Pow(MaxErr/err, 1./2.))
		setLastErr(err)
		setMaxTorque(dy)
	} else {
		// undo bad step
		util.Assert(FixDt == 0)
		Time -= Dt_si
		cuda.Madd2(y, y, dy0, 1, -dt)
		NUndone++
		adaptDt(math.Pow(MaxErr/err, 1./3.))
	}
}
예제 #10
0
파일: resample.go 프로젝트: kyeongdong/3
// Downsample returns a slice of new size N, smaller than in.Size().
// Averaging interpolation over the input slice.
// in is returned untouched if the sizes are equal.
func Downsample(In [][][][]float32, N [3]int) [][][][]float32 {
	if SizeOf(In[0]) == N {
		return In // nothing to do
	}

	nComp := len(In)
	out := NewSlice(nComp, N)
	Out := out.Tensors()

	srcsize := SizeOf(In[0])
	dstsize := SizeOf(Out[0])

	Dx := dstsize[X]
	Dy := dstsize[Y]
	Dz := dstsize[Z]
	Sx := srcsize[X]
	Sy := srcsize[Y]
	Sz := srcsize[Z]
	scalex := Sx / Dx
	scaley := Sy / Dy
	scalez := Sz / Dz
	util.Assert(scalex > 0 && scaley > 0)

	for c := range Out {

		for iz := 0; iz < Dz; iz++ {
			for iy := 0; iy < Dy; iy++ {
				for ix := 0; ix < Dx; ix++ {
					sum, n := 0.0, 0.0

					for I := 0; I < scalez; I++ {
						i2 := iz*scalez + I
						for J := 0; J < scaley; J++ {
							j2 := iy*scaley + J
							for K := 0; K < scalex; K++ {
								k2 := ix*scalex + K

								if i2 < Sz && j2 < Sy && k2 < Sx {
									sum += float64(In[c][i2][j2][k2])
									n++
								}
							}
						}
					}
					Out[c][iz][iy][ix] = float32(sum / n)
				}
			}
		}
	}

	return Out
}
예제 #11
0
파일: demagkernel.go 프로젝트: callistoaz/3
// Calculates the magnetostatic kernel by brute-force integration
// of magnetic charges over the faces and averages over cell volumes.
func CalcDemagKernel(inputSize, pbc [3]int, cellsize [3]float64, accuracy float64) (kernel [3][3]*data.Slice) {

	// Add zero-padding in non-PBC directions
	size := padSize(inputSize, pbc)

	// Sanity check
	{
		util.Assert(size[Z] > 0 && size[Y] > 0 && size[X] > 0)
		util.Assert(cellsize[X] > 0 && cellsize[Y] > 0 && cellsize[Z] > 0)
		util.Assert(pbc[X] >= 0 && pbc[Y] >= 0 && pbc[Z] >= 0)
		util.Assert(accuracy > 0)
	}

	// Allocate only upper diagonal part. The rest is symmetric due to reciprocity.
	var array [3][3][][][]float32
	for i := 0; i < 3; i++ {
		for j := i; j < 3; j++ {
			kernel[i][j] = data.NewSlice(1, size)
			array[i][j] = kernel[i][j].Scalars()
		}
	}

	// Field (destination) loop ranges
	r1, r2 := kernelRanges(size, pbc)

	// smallest cell dimension is our typical length scale
	L := cellsize[X]
	{
		if cellsize[Y] < L {
			L = cellsize[Y]
		}
		if cellsize[Z] < L {
			L = cellsize[Z]
		}
	}

	progress, progmax := 0, (1+(r2[Y]-r1[Y]))*(1+(r2[Z]-r1[Z])) // progress bar
	done := make(chan struct{}, 3)                              // parallel calculation of one component done?

	// Start brute integration
	// 9 nested loops, does that stress you out?
	// Fortunately, the 5 inner ones usually loop over just one element.

	for s := 0; s < 3; s++ { // source index Ksdxyz (parallelized over)
		go func(s int) {
			u, v, w := s, (s+1)%3, (s+2)%3 // u = direction of source (s), v & w are the orthogonal directions
			var (
				R, R2  [3]float64 // field and source cell center positions
				pole   [3]float64 // position of point charge on the surface
				points int        // counts used integration points
			)

			for z := r1[Z]; z <= r2[Z]; z++ {
				zw := wrap(z, size[Z])
				// skip one half, reconstruct from symmetry later
				// check on wrapped index instead of loop range so it also works for PBC
				if zw > size[Z]/2 {
					if s == 0 {
						progress += (1 + (r2[Y] - r1[Y]))
					}
					continue
				}
				R[Z] = float64(z) * cellsize[Z]

				for y := r1[Y]; y <= r2[Y]; y++ {

					if s == 0 { // show progress of only one component
						progress++
						util.Progress(progress, progmax, "Calculating demag kernel")
					}

					yw := wrap(y, size[Y])
					if yw > size[Y]/2 {
						continue
					}
					R[Y] = float64(y) * cellsize[Y]

					for x := r1[X]; x <= r2[X]; x++ {
						xw := wrap(x, size[X])
						if xw > size[X]/2 {
							continue
						}
						R[X] = float64(x) * cellsize[X]

						// choose number of integration points depending on how far we are from source.
						dx, dy, dz := delta(x)*cellsize[X], delta(y)*cellsize[Y], delta(z)*cellsize[Z]
						d := math.Sqrt(dx*dx + dy*dy + dz*dz)
						if d == 0 {
							d = L
						}
						maxSize := d / accuracy // maximum acceptable integration size

						nv := int(math.Max(cellsize[v]/maxSize, 1) + 0.5)
						nw := int(math.Max(cellsize[w]/maxSize, 1) + 0.5)
						nx := int(math.Max(cellsize[X]/maxSize, 1) + 0.5)
						ny := int(math.Max(cellsize[Y]/maxSize, 1) + 0.5)
						nz := int(math.Max(cellsize[Z]/maxSize, 1) + 0.5)
						// Stagger source and destination grids.
						// Massively improves accuracy, see note.
						nv *= 2
						nw *= 2

						util.Assert(nv > 0 && nw > 0 && nx > 0 && ny > 0 && nz > 0)

						scale := 1 / float64(nv*nw*nx*ny*nz)
						surface := cellsize[v] * cellsize[w] // the two directions perpendicular to direction s
						charge := surface * scale
						pu1 := cellsize[u] / 2. // positive pole center
						pu2 := -pu1             // negative pole center

						// Do surface integral over source cell, accumulate  in B
						var B [3]float64
						for i := 0; i < nv; i++ {
							pv := -(cellsize[v] / 2.) + cellsize[v]/float64(2*nv) + float64(i)*(cellsize[v]/float64(nv))
							pole[v] = pv
							for j := 0; j < nw; j++ {
								pw := -(cellsize[w] / 2.) + cellsize[w]/float64(2*nw) + float64(j)*(cellsize[w]/float64(nw))
								pole[w] = pw

								// Do volume integral over destination cell
								for α := 0; α < nx; α++ {
									rx := R[X] - cellsize[X]/2 + cellsize[X]/float64(2*nx) + (cellsize[X]/float64(nx))*float64(α)

									for β := 0; β < ny; β++ {
										ry := R[Y] - cellsize[Y]/2 + cellsize[Y]/float64(2*ny) + (cellsize[Y]/float64(ny))*float64(β)

										for γ := 0; γ < nz; γ++ {
											rz := R[Z] - cellsize[Z]/2 + cellsize[Z]/float64(2*nz) + (cellsize[Z]/float64(nz))*float64(γ)
											points++

											pole[u] = pu1
											R2[X], R2[Y], R2[Z] = rx-pole[X], ry-pole[Y], rz-pole[Z]
											r := math.Sqrt(R2[X]*R2[X] + R2[Y]*R2[Y] + R2[Z]*R2[Z])
											qr := charge / (4 * math.Pi * r * r * r)
											bx := R2[X] * qr
											by := R2[Y] * qr
											bz := R2[Z] * qr

											pole[u] = pu2
											R2[X], R2[Y], R2[Z] = rx-pole[X], ry-pole[Y], rz-pole[Z]
											r = math.Sqrt(R2[X]*R2[X] + R2[Y]*R2[Y] + R2[Z]*R2[Z])
											qr = -charge / (4 * math.Pi * r * r * r)
											B[X] += (bx + R2[X]*qr) // addition ordered for accuracy
											B[Y] += (by + R2[Y]*qr)
											B[Z] += (bz + R2[Z]*qr)

										}
									}
								}
							}
						}
						for d := s; d < 3; d++ { // destination index Ksdxyz
							array[s][d][zw][yw][xw] += float32(B[d]) // += needed in case of PBC
						}
					}
				}
			}
			done <- struct{}{} // notify parallel computation of this component is done
		}(s)
	}
	// wait for all 3 components to finish
	<-done
	<-done
	<-done

	// Reconstruct skipped parts from symmetry (X)
	for z := 0; z < size[Z]; z++ {
		for y := 0; y < size[Y]; y++ {
			for x := size[X]/2 + 1; x < size[X]; x++ {
				x2 := size[X] - x
				array[X][X][z][y][x] = array[X][X][z][y][x2]
				array[X][Y][z][y][x] = -array[X][Y][z][y][x2]
				array[X][Z][z][y][x] = -array[X][Z][z][y][x2]
				array[Y][Y][z][y][x] = array[Y][Y][z][y][x2]
				array[Y][Z][z][y][x] = array[Y][Z][z][y][x2]
				array[Z][Z][z][y][x] = array[Z][Z][z][y][x2]
			}
		}
	}

	// Reconstruct skipped parts from symmetry (Y)
	for z := 0; z < size[Z]; z++ {
		for y := size[Y]/2 + 1; y < size[Y]; y++ {
			y2 := size[Y] - y
			for x := 0; x < size[X]; x++ {
				array[X][X][z][y][x] = array[X][X][z][y2][x]
				array[X][Y][z][y][x] = -array[X][Y][z][y2][x]
				array[X][Z][z][y][x] = array[X][Z][z][y2][x]
				array[Y][Y][z][y][x] = array[Y][Y][z][y2][x]
				array[Y][Z][z][y][x] = -array[Y][Z][z][y2][x]
				array[Z][Z][z][y][x] = array[Z][Z][z][y2][x]

			}
		}
	}

	// Reconstruct skipped parts from symmetry (Z)
	for z := size[Z]/2 + 1; z < size[Z]; z++ {
		z2 := size[Z] - z
		for y := 0; y < size[Y]; y++ {
			for x := 0; x < size[X]; x++ {
				array[X][X][z][y][x] = array[X][X][z2][y][x]
				array[X][Y][z][y][x] = array[X][Y][z2][y][x]
				array[X][Z][z][y][x] = -array[X][Z][z2][y][x]
				array[Y][Y][z][y][x] = array[Y][Y][z2][y][x]
				array[Y][Z][z][y][x] = -array[Y][Z][z2][y][x]
				array[Z][Z][z][y][x] = array[Z][Z][z2][y][x]
			}
		}
	}

	// for 2D these elements are zero:
	if size[Z] == 1 {
		kernel[X][Z] = nil
		kernel[Y][Z] = nil
	}
	// make result symmetric for tools that expect it so.
	kernel[Y][X] = kernel[X][Y]
	kernel[Z][X] = kernel[X][Z]
	kernel[Z][Y] = kernel[Y][Z]
	return kernel
}
예제 #12
0
파일: conv_demag.go 프로젝트: markhyq/3
func (c *DemagConvolution) init(realKern [3][3]*data.Slice) {
	// init device buffers
	// 2D re-uses fftBuf[X] as fftBuf[Z], 3D needs all 3 fftBufs.
	nc := fftR2COutputSizeFloats(c.realKernSize)
	c.fftCBuf[X] = NewSlice(1, nc)
	c.fftCBuf[Y] = NewSlice(1, nc)
	if c.is2D() {
		c.fftCBuf[Z] = c.fftCBuf[X]
	} else {
		c.fftCBuf[Z] = NewSlice(1, nc)
	}
	// Real buffer shares storage with Complex buffer
	for i := 0; i < 3; i++ {
		c.fftRBuf[i] = data.SliceFromPtrs(c.realKernSize, data.GPUMemory, []unsafe.Pointer{c.fftCBuf[i].DevPtr(0)})
	}

	// init FFT plans
	c.fwPlan = newFFT3DR2C(c.realKernSize[X], c.realKernSize[Y], c.realKernSize[Z])
	c.bwPlan = newFFT3DC2R(c.realKernSize[X], c.realKernSize[Y], c.realKernSize[Z])

	// init FFT kernel

	// logic size of FFT(kernel): store real parts only
	c.fftKernLogicSize = fftR2COutputSizeFloats(c.realKernSize)
	util.Assert(c.fftKernLogicSize[X]%2 == 0)
	c.fftKernLogicSize[X] /= 2

	// physical size of FFT(kernel): store only non-redundant part exploiting Y, Z mirror symmetry
	// X mirror symmetry already exploited: FFT(kernel) is purely real.
	physKSize := [3]int{c.fftKernLogicSize[X], c.fftKernLogicSize[Y]/2 + 1, c.fftKernLogicSize[Z]/2 + 1}

	output := c.fftCBuf[0]
	input := c.fftRBuf[0]
	fftKern := data.NewSlice(1, physKSize)
	kfull := data.NewSlice(1, output.Size()) // not yet exploiting symmetry
	kfulls := kfull.Scalars()
	kCSize := physKSize
	kCSize[X] *= 2                     // size of kernel after removing Y,Z redundant parts, but still complex
	kCmplx := data.NewSlice(1, kCSize) // not yet exploiting X symmetry
	kc := kCmplx.Scalars()

	for i := 0; i < 3; i++ {
		for j := i; j < 3; j++ { // upper triangular part
			if realKern[i][j] != nil { // ignore 0's
				// FW FFT
				data.Copy(input, realKern[i][j])
				c.fwPlan.ExecAsync(input, output)
				data.Copy(kfull, output)

				// extract non-redundant part (Y,Z symmetry)
				for iz := 0; iz < kCSize[Z]; iz++ {
					for iy := 0; iy < kCSize[Y]; iy++ {
						for ix := 0; ix < kCSize[X]; ix++ {
							kc[iz][iy][ix] = kfulls[iz][iy][ix]
						}
					}
				}

				// extract real parts (X symmetry)
				scaleRealParts(fftKern, kCmplx, 1/float32(c.fwPlan.InputLen()))
				c.kern[i][j] = GPUCopy(fftKern)
			}
		}
	}
}
예제 #13
0
파일: rk4.go 프로젝트: kyeongdong/3
func (rk *RK4) Step() {
	m := M.Buffer()
	size := m.Size()

	if FixDt != 0 {
		Dt_si = FixDt
	}

	t0 := Time
	// backup magnetization
	m0 := cuda.Buffer(3, size)
	defer cuda.Recycle(m0)
	data.Copy(m0, m)

	k1, k2, k3, k4 := cuda.Buffer(3, size), cuda.Buffer(3, size), cuda.Buffer(3, size), cuda.Buffer(3, size)

	defer cuda.Recycle(k1)
	defer cuda.Recycle(k2)
	defer cuda.Recycle(k3)
	defer cuda.Recycle(k4)

	h := float32(Dt_si * GammaLL) // internal time step = Dt * gammaLL

	// stage 1
	torqueFn(k1)

	// stage 2
	Time = t0 + (1./2.)*Dt_si
	cuda.Madd2(m, m, k1, 1, (1./2.)*h) // m = m*1 + k1*h/2
	M.normalize()
	torqueFn(k2)

	// stage 3
	cuda.Madd2(m, m0, k2, 1, (1./2.)*h) // m = m0*1 + k2*1/2
	M.normalize()
	torqueFn(k3)

	// stage 4
	Time = t0 + Dt_si
	cuda.Madd2(m, m0, k3, 1, 1.*h) // m = m0*1 + k3*1
	M.normalize()
	torqueFn(k4)

	err := cuda.MaxVecDiff(k1, k4) * float64(h)

	// adjust next time step
	if err < MaxErr || Dt_si <= MinDt || FixDt != 0 { // mindt check to avoid infinite loop
		// step OK
		// 4th order solution
		madd5(m, m0, k1, k2, k3, k4, 1, (1./6.)*h, (1./3.)*h, (1./3.)*h, (1./6.)*h)
		M.normalize()
		NSteps++
		adaptDt(math.Pow(MaxErr/err, 1./4.))
		setLastErr(err)
		setMaxTorque(k4)
	} else {
		// undo bad step
		//util.Println("Bad step at t=", t0, ", err=", err)
		util.Assert(FixDt == 0)
		Time = t0
		data.Copy(m, m0)
		NUndone++
		adaptDt(math.Pow(MaxErr/err, 1./5.))
	}
}
예제 #14
0
파일: rk45dp.go 프로젝트: kyeongdong/3
func (rk *RK45DP) Step() {
	m := M.Buffer()
	size := m.Size()

	if FixDt != 0 {
		Dt_si = FixDt
	}

	// upon resize: remove wrongly sized k1
	if rk.k1.Size() != m.Size() {
		rk.Free()
	}

	// first step ever: one-time k1 init and eval
	if rk.k1 == nil {
		rk.k1 = cuda.NewSlice(3, size)
		torqueFn(rk.k1)
	}

	// FSAL cannot be used with finite temperature
	if !Temp.isZero() {
		torqueFn(rk.k1)
	}

	t0 := Time
	// backup magnetization
	m0 := cuda.Buffer(3, size)
	defer cuda.Recycle(m0)
	data.Copy(m0, m)

	k2, k3, k4, k5, k6 := cuda.Buffer(3, size), cuda.Buffer(3, size), cuda.Buffer(3, size), cuda.Buffer(3, size), cuda.Buffer(3, size)
	defer cuda.Recycle(k2)
	defer cuda.Recycle(k3)
	defer cuda.Recycle(k4)
	defer cuda.Recycle(k5)
	defer cuda.Recycle(k6)
	// k2 will be re-used as k7

	h := float32(Dt_si * GammaLL) // internal time step = Dt * gammaLL

	// there is no explicit stage 1: k1 from previous step

	// stage 2
	Time = t0 + (1./5.)*Dt_si
	cuda.Madd2(m, m, rk.k1, 1, (1./5.)*h) // m = m*1 + k1*h/5
	M.normalize()
	torqueFn(k2)

	// stage 3
	Time = t0 + (3./10.)*Dt_si
	cuda.Madd3(m, m0, rk.k1, k2, 1, (3./40.)*h, (9./40.)*h)
	M.normalize()
	torqueFn(k3)

	// stage 4
	Time = t0 + (4./5.)*Dt_si
	madd4(m, m0, rk.k1, k2, k3, 1, (44./45.)*h, (-56./15.)*h, (32./9.)*h)
	M.normalize()
	torqueFn(k4)

	// stage 5
	Time = t0 + (8./9.)*Dt_si
	madd5(m, m0, rk.k1, k2, k3, k4, 1, (19372./6561.)*h, (-25360./2187.)*h, (64448./6561.)*h, (-212./729.)*h)
	M.normalize()
	torqueFn(k5)

	// stage 6
	Time = t0 + (1.)*Dt_si
	madd6(m, m0, rk.k1, k2, k3, k4, k5, 1, (9017./3168.)*h, (-355./33.)*h, (46732./5247.)*h, (49./176.)*h, (-5103./18656.)*h)
	M.normalize()
	torqueFn(k6)

	// stage 7: 5th order solution
	Time = t0 + (1.)*Dt_si
	// no k2
	madd6(m, m0, rk.k1, k3, k4, k5, k6, 1, (35./384.)*h, (500./1113.)*h, (125./192.)*h, (-2187./6784.)*h, (11./84.)*h) // 5th
	M.normalize()
	k7 := k2     // re-use k2
	torqueFn(k7) // next torque if OK

	// error estimate
	Err := cuda.Buffer(3, size) //k3 // re-use k3 as error estimate
	defer cuda.Recycle(Err)
	madd6(Err, rk.k1, k3, k4, k5, k6, k7, (35./384.)-(5179./57600.), (500./1113.)-(7571./16695.), (125./192.)-(393./640.), (-2187./6784.)-(-92097./339200.), (11./84.)-(187./2100.), (0.)-(1./40.))

	// determine error
	err := cuda.MaxVecNorm(Err) * float64(h)

	// adjust next time step
	if err < MaxErr || Dt_si <= MinDt || FixDt != 0 { // mindt check to avoid infinite loop
		// step OK
		setLastErr(err)
		setMaxTorque(k7)
		NSteps++
		Time = t0 + Dt_si
		adaptDt(math.Pow(MaxErr/err, 1./5.))
		data.Copy(rk.k1, k7) // FSAL
	} else {
		// undo bad step
		//util.Println("Bad step at t=", t0, ", err=", err)
		util.Assert(FixDt == 0)
		Time = t0
		data.Copy(m, m0)
		NUndone++
		adaptDt(math.Pow(MaxErr/err, 1./6.))
	}
}
예제 #15
0
파일: util.go 프로젝트: kyeongdong/3
func unslice(v []float64) [3]float64 {
	util.Assert(len(v) == 3)
	return [3]float64{v[0], v[1], v[2]}
}
예제 #16
0
파일: util.go 프로젝트: kyeongdong/3
// dst = a/b, unless b == 0
func paramDiv(dst, a, b [][NREGION]float32) {
	util.Assert(len(dst) == 1 && len(a) == 1 && len(b) == 1)
	for i := 0; i < NREGION; i++ { // not regions.maxreg
		dst[0][i] = safediv(a[0][i], b[0][i])
	}
}
예제 #17
0
파일: rk23.go 프로젝트: kyeongdong/3
func (rk *RK23) Step() {
	m := M.Buffer()
	size := m.Size()

	if FixDt != 0 {
		Dt_si = FixDt
	}

	// upon resize: remove wrongly sized k1
	if rk.k1.Size() != m.Size() {
		rk.Free()
	}

	// first step ever: one-time k1 init and eval
	if rk.k1 == nil {
		rk.k1 = cuda.NewSlice(3, size)
		torqueFn(rk.k1)
	}

	// FSAL cannot be used with temperature
	if !Temp.isZero() {
		torqueFn(rk.k1)
	}

	t0 := Time
	// backup magnetization
	m0 := cuda.Buffer(3, size)
	defer cuda.Recycle(m0)
	data.Copy(m0, m)

	k2, k3, k4 := cuda.Buffer(3, size), cuda.Buffer(3, size), cuda.Buffer(3, size)
	defer cuda.Recycle(k2)
	defer cuda.Recycle(k3)
	defer cuda.Recycle(k4)

	h := float32(Dt_si * GammaLL) // internal time step = Dt * gammaLL

	// there is no explicit stage 1: k1 from previous step

	// stage 2
	Time = t0 + (1./2.)*Dt_si
	cuda.Madd2(m, m, rk.k1, 1, (1./2.)*h) // m = m*1 + k1*h/2
	M.normalize()
	torqueFn(k2)

	// stage 3
	Time = t0 + (3./4.)*Dt_si
	cuda.Madd2(m, m0, k2, 1, (3./4.)*h) // m = m0*1 + k2*3/4
	M.normalize()
	torqueFn(k3)

	// 3rd order solution
	madd4(m, m0, rk.k1, k2, k3, 1, (2./9.)*h, (1./3.)*h, (4./9.)*h)
	M.normalize()

	// error estimate
	Time = t0 + Dt_si
	torqueFn(k4)
	Err := k2 // re-use k2 as error
	// difference of 3rd and 2nd order torque without explicitly storing them first
	madd4(Err, rk.k1, k2, k3, k4, (7./24.)-(2./9.), (1./4.)-(1./3.), (1./3.)-(4./9.), (1. / 8.))

	// determine error
	err := cuda.MaxVecNorm(Err) * float64(h)

	// adjust next time step
	if err < MaxErr || Dt_si <= MinDt || FixDt != 0 { // mindt check to avoid infinite loop
		// step OK
		setLastErr(err)
		setMaxTorque(k4)
		NSteps++
		Time = t0 + Dt_si
		adaptDt(math.Pow(MaxErr/err, 1./3.))
		data.Copy(rk.k1, k4) // FSAL
	} else {
		// undo bad step
		//util.Println("Bad step at t=", t0, ", err=", err)
		util.Assert(FixDt == 0)
		Time = t0
		data.Copy(m, m0)
		NUndone++
		adaptDt(math.Pow(MaxErr/err, 1./4.))
	}
}
예제 #18
0
파일: excitation.go 프로젝트: jsampaio/3
func (p *Excitation) MSlice() cuda.MSlice {
	buf, r := p.Slice()
	util.Assert(r == true)
	return cuda.ToMSlice(buf)
}
예제 #19
0
파일: mfmkernel.go 프로젝트: kyeongdong/3
// Kernel for the vertical derivative of the force on an MFM tip due to mx, my, mz.
// This is the 2nd derivative of the energy w.r.t. z.
func MFMKernel(mesh *d.Mesh, lift, tipsize float64) (kernel [3]*d.Slice) {

	const TipCharge = 1 / Mu0 // tip charge
	const Δ = 1e-9            // tip oscillation, take 2nd derivative over this distance
	util.AssertMsg(lift > 0, "MFM tip crashed into sample, please lift the new one higher")

	{ // Kernel mesh is 2x larger than input, instead in case of PBC
		pbc := mesh.PBC()
		sz := padSize(mesh.Size(), pbc)
		cs := mesh.CellSize()
		mesh = d.NewMesh(sz[X], sz[Y], sz[Z], cs[X], cs[Y], cs[Z], pbc[:]...)
	}

	// Shorthand
	size := mesh.Size()
	pbc := mesh.PBC()
	cellsize := mesh.CellSize()
	volume := cellsize[X] * cellsize[Y] * cellsize[Z]
	fmt.Println("calculating MFM kernel")

	// Sanity check
	{
		util.Assert(size[Z] >= 1 && size[Y] >= 2 && size[X] >= 2)
		util.Assert(cellsize[X] > 0 && cellsize[Y] > 0 && cellsize[Z] > 0)
		util.AssertMsg(size[X]%2 == 0 && size[Y]%2 == 0, "Even kernel size needed")
		if size[Z] > 1 {
			util.AssertMsg(size[Z]%2 == 0, "Even kernel size needed")
		}
	}

	// Allocate only upper diagonal part. The rest is symmetric due to reciprocity.
	var K [3][][][]float32
	for i := 0; i < 3; i++ {
		kernel[i] = d.NewSlice(1, mesh.Size())
		K[i] = kernel[i].Scalars()
	}

	r1, r2 := kernelRanges(size, pbc)
	progress, progmax := 0, (1+r2[Y]-r1[Y])*(1+r2[Z]-r1[Z])

	for iz := r1[Z]; iz <= r2[Z]; iz++ {
		zw := wrap(iz, size[Z])
		z := float64(iz) * cellsize[Z]

		for iy := r1[Y]; iy <= r2[Y]; iy++ {
			yw := wrap(iy, size[Y])
			y := float64(iy) * cellsize[Y]
			progress++
			util.Progress(progress, progmax, "Calculating MFM kernel")

			for ix := r1[X]; ix <= r2[X]; ix++ {
				x := float64(ix) * cellsize[X]
				xw := wrap(ix, size[X])

				for s := 0; s < 3; s++ { // source index Ksxyz
					m := d.Vector{0, 0, 0}
					m[s] = 1

					var E [3]float64 // 3 energies for 2nd derivative

					for i := -1; i <= 1; i++ {
						I := float64(i)
						R := d.Vector{-x, -y, z - (lift + (I * Δ))}
						r := R.Len()
						B := R.Mul(TipCharge / (4 * math.Pi * r * r * r))

						R = d.Vector{-x, -y, z - (lift + tipsize + (I * Δ))}
						r = R.Len()
						B = B.Add(R.Mul(-TipCharge / (4 * math.Pi * r * r * r)))

						E[i+1] = B.Dot(m) * volume // i=-1 stored in  E[0]
					}

					dFdz_tip := ((E[0] - E[1]) + (E[2] - E[1])) / (Δ * Δ) // dFz/dz = d2E/dz2

					K[s][zw][yw][xw] += float32(dFdz_tip) // += needed in case of PBC
				}
			}
		}
	}

	return kernel
}
예제 #20
0
파일: lutdata.go 프로젝트: kyeongdong/3
// utility for LUT of single-component data
func (p *lut) gpuLUT1() cuda.LUTPtr {
	util.Assert(len(p.gpu_buf) == 1)
	return cuda.LUTPtr(p.gpuLUT()[0])
}