Exemple #1
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// Exercise, p. 136.
func TestPosition(t *testing.T) {
	eqFrom := &coord.Equatorial{
		base.NewRA(2, 31, 48.704).Rad(),
		base.NewAngle(false, 89, 15, 50.72).Rad(),
	}
	eqTo := &coord.Equatorial{}
	mα := base.NewHourAngle(false, 0, 0, 0.19877)
	mδ := base.NewAngle(true, 0, 0, 0.0152)
	for _, tc := range []struct {
		α, δ string
		jde  float64
	}{
		{"1 22 33.90", "88 46 26.18", base.BesselianYearToJDE(1900)},
		{"3 48 16.43", "89 27 15.38", base.JulianYearToJDE(2050)},
		{"5 53 29.17", "89 32 22.18", base.JulianYearToJDE(2100)},
	} {
		epochTo := base.JDEToJulianYear(tc.jde)
		precess.Position(eqFrom, eqTo, 2000.0, epochTo, mα, mδ)
		αStr := fmt.Sprintf("%.2x", base.NewFmtRA(eqTo.RA))
		δStr := fmt.Sprintf("%.2x", base.NewFmtAngle(eqTo.Dec))
		if αStr != tc.α {
			t.Fatal("got:", αStr, "want:", tc.α)
		}
		if δStr != tc.δ {
			t.Fatal(δStr)
		}
	}
}
Exemple #2
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func TestPrecessor_Precess(t *testing.T) {
	// Exercise, p. 136.
	eqFrom := &coord.Equatorial{
		RA:  base.NewRA(2, 31, 48.704).Rad(),
		Dec: base.NewAngle(false, 89, 15, 50.72).Rad(),
	}
	mα := base.NewHourAngle(false, 0, 0, .19877)
	mδ := base.NewAngle(false, 0, 0, -.0152)
	epochs := []float64{
		base.JDEToJulianYear(base.B1900),
		2050,
		2100,
	}
	answer := []string{
		"α = 1ʰ22ᵐ33ˢ.90   δ = +88°46′26″.18",
		"α = 3ʰ48ᵐ16ˢ.43   δ = +89°27′15″.38",
		"α = 5ʰ53ᵐ29ˢ.17   δ = +89°32′22″.18",
	}
	eqTo := &coord.Equatorial{}
	for i, epochTo := range epochs {
		precess.Position(eqFrom, eqTo, 2000, epochTo, mα, mδ)
		if answer[i] != fmt.Sprintf("α = %0.2d   δ = %+0.2d",
			base.NewFmtRA(eqTo.RA), base.NewFmtAngle(eqTo.Dec)) {
			t.Fatal(i)
		}
	}
}
Exemple #3
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func ExampleProperMotion3D() {
	// Example 21.d, p. 141.
	eqFrom := &coord.Equatorial{
		RA:  base.NewRA(6, 45, 8.871).Rad(),
		Dec: base.NewAngle(true, 16, 42, 57.99).Rad(),
	}
	mra := base.NewHourAngle(false, 0, 0, -0.03847)
	mdec := base.NewAngle(false, 0, 0, -1.2053)
	r := 2.64           // given in correct unit
	mr := -7.6 / 977792 // magic conversion factor
	eqTo := &coord.Equatorial{}
	fmt.Printf("Δr = %.9f, Δα = %.10f, Δδ = %.10f\n", mr, mra, mdec)
	for _, epoch := range []float64{1000, 0, -1000, -2000, -10000} {
		precess.ProperMotion3D(eqFrom, eqTo, 2000, epoch, r, mr, mra, mdec)
		fmt.Printf("%8.1f  %0.2d  %-0.1d\n", epoch,
			base.NewFmtRA(eqTo.RA), base.NewFmtAngle(eqTo.Dec))
	}
	// Output:
	// Δr = -0.000007773, Δα = -0.0000027976, Δδ = -0.0000058435
	//   1000.0  6ʰ45ᵐ47ˢ.16  -16°22′56″.0
	//      0.0  6ʰ46ᵐ25ˢ.09  -16°03′00″.8
	//  -1000.0  6ʰ47ᵐ02ˢ.67  -15°43′12″.3
	//  -2000.0  6ʰ47ᵐ39ˢ.91  -15°23′30″.6
	// -10000.0  6ʰ52ᵐ25ˢ.72  -12°50′06″.7
}
Exemple #4
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func ExampleElements_Position() {
	// Example 33.b, p. 232.
	earth, err := pp.LoadPlanet(pp.Earth, "")
	if err != nil {
		fmt.Println(err)
		return
	}
	k := &elliptic.Elements{
		TimeP: julian.CalendarGregorianToJD(1990, 10, 28.54502),
		Axis:  2.2091404,
		Ecc:   .8502196,
		Inc:   11.94524 * math.Pi / 180,
		Node:  334.75006 * math.Pi / 180,
		ArgP:  186.23352 * math.Pi / 180,
	}
	j := julian.CalendarGregorianToJD(1990, 10, 6)
	α, δ, ψ := k.Position(j, earth)
	fmt.Printf("α = %.1d\n", base.NewFmtRA(α))
	fmt.Printf("δ = %.0d\n", base.NewFmtAngle(δ))
	fmt.Printf("ψ = %.2f\n", ψ*180/math.Pi)
	// Output:
	// α = 10ʰ34ᵐ14ˢ.2
	// δ = 19°9′31″
	// ψ = 40.51
}
Exemple #5
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func ExampleApparentEquatorial() {
	// Example 25.a, p. 165.
	jde := julian.CalendarGregorianToJD(1992, 10, 13)
	α, δ := solar.ApparentEquatorial(jde)
	fmt.Printf("α: %.1d\n", base.NewFmtRA(α))
	fmt.Printf("δ: %d\n", base.NewFmtAngle(δ))
	// Output:
	// α: 13ʰ13ᵐ31ˢ.4
	// δ: -7°47′6″
}
Exemple #6
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func ExampleStellar() {
	// Exercise, p. 119.
	day1 := 7.
	day5 := 27.
	r2 := []float64{
		base.NewRA(15, 3, 51.937).Rad(),
		base.NewRA(15, 9, 57.327).Rad(),
		base.NewRA(15, 15, 37.898).Rad(),
		base.NewRA(15, 20, 50.632).Rad(),
		base.NewRA(15, 25, 32.695).Rad(),
	}
	d2 := []float64{
		base.NewAngle(true, 8, 57, 34.51).Rad(),
		base.NewAngle(true, 9, 9, 03.88).Rad(),
		base.NewAngle(true, 9, 17, 37.94).Rad(),
		base.NewAngle(true, 9, 23, 16.25).Rad(),
		base.NewAngle(true, 9, 26, 01.01).Rad(),
	}
	jd := julian.CalendarGregorianToJD(1996, 2, 17)
	dt := jd - base.J2000
	dy := dt / base.JulianYear
	dc := dy / 100
	fmt.Printf("%.2f years\n", dy)
	fmt.Printf("%.4f century\n", dc)

	pmr := -.649 // sec/cen
	pmd := -1.91 // sec/cen
	r1 := base.NewRA(15, 17, 0.421+pmr*dc).Rad()
	// Careful with quick and dirty way of applying correction to seconds
	// component before converting to radians.  The dec here is negative
	// so correction must be subtracted.  Alternative, less error-prone,
	// way would be to convert both to radians, then add.
	d1 := base.NewAngle(true, 9, 22, 58.54-pmd*dc).Rad()
	fmt.Printf("α′ = %.3d, δ′ = %.2d\n",
		base.NewFmtRA(r1), base.NewFmtAngle(d1))

	day, dd, err := conjunction.Stellar(day1, day5, r1, d1, r2, d2)
	if err != nil {
		fmt.Println(err)
		return
	}
	fmt.Println(base.NewFmtAngle(dd))
	dInt, dFrac := math.Modf(day)
	fmt.Printf("1996 February %d at %s TD\n", int(dInt),
		base.NewFmtTime(dFrac*24*3600))

	// Output:
	// -3.87 years
	// -0.0387 century
	// α′ = 15ʰ17ᵐ0ˢ.446, δ′ = -9°22′58″.47
	// 3′38″
	// 1996 February 18 at 6ʰ36ᵐ55ˢ TD
}
Exemple #7
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func ExampleTopocentric() {
	// Example 40.a, p. 280
	α, δ := parallax.Topocentric(339.530208*math.Pi/180,
		-15.771083*math.Pi/180,
		.37276, .546861, .836339,
		base.NewHourAngle(false, 7, 47, 27).Rad(),
		julian.CalendarGregorianToJD(2003, 8, 28+(3+17./60)/24))
	fmt.Printf("α' = %.2d\n", base.NewFmtRA(α))
	fmt.Printf("δ' = %.1d\n", base.NewFmtAngle(δ))
	// Output:
	// α' = 22ʰ38ᵐ8ˢ.54
	// δ' = -15°46′30″.0
}
Exemple #8
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func ExampleAstrometric() {
	// Example 37.a, p. 266
	e, err := pp.LoadPlanet(pp.Earth, "")
	if err != nil {
		fmt.Println(err)
		return
	}
	α, δ := pluto.Astrometric(2448908.5, e)
	fmt.Printf("α: %.1d\n", base.NewFmtRA(α))
	fmt.Printf("δ: %.0d\n", base.NewFmtAngle(δ))
	// Output:
	// α: 15ʰ31ᵐ43ˢ.8
	// δ: -4°27′29″
}
Exemple #9
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func ExampleLen4Half() {
	// Example 3.f, p. 32.
	half, err := interp.Len4Half([]float64{
		base.NewRA(10, 18, 48.732).Rad(),
		base.NewRA(10, 23, 22.835).Rad(),
		base.NewRA(10, 27, 57.247).Rad(),
		base.NewRA(10, 32, 31.983).Rad(),
	})
	if err != nil {
		fmt.Println(err)
		return
	}
	fmt.Printf("%.3d", base.NewFmtRA(half))
	// Output:
	// 10ʰ25ᵐ40ˢ.001
}
Exemple #10
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func ExamplePositionRonVondrak() {
	// Example 23.b, p. 156
	jd := julian.CalendarGregorianToJD(2028, 11, 13.19)
	eq := &coord.Equatorial{
		RA:  base.NewRA(2, 44, 11.986).Rad(),
		Dec: base.NewAngle(false, 49, 13, 42.48).Rad(),
	}
	apparent.PositionRonVondrak(eq, eq, base.JDEToJulianYear(jd),
		base.NewHourAngle(false, 0, 0, 0.03425),
		base.NewAngle(true, 0, 0, 0.0895))
	fmt.Printf("α = %0.3d\n", base.NewFmtRA(eq.RA))
	fmt.Printf("δ = %0.2d\n", base.NewFmtAngle(eq.Dec))
	// Output:
	// α = 2ʰ46ᵐ14ˢ.392
	// δ = 49°21′07″.45
}
Exemple #11
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func ExampleApparentEquatorialVSOP87() {
	// Example 25.b, p. 169, but as this code uses the full VSOP87 theory,
	// results match those at bottom of p. 165.
	e, err := pp.LoadPlanet(pp.Earth, "")
	if err != nil {
		fmt.Println(err)
		return
	}
	jde := julian.CalendarGregorianToJD(1992, 10, 13)
	α, δ, _ := solar.ApparentEquatorialVSOP87(e, jde)
	fmt.Printf("α: %.3d\n", base.NewFmtRA(α))
	fmt.Printf("δ: %+.2d\n", base.NewFmtAngle(δ))
	// Output:
	// α: 13ʰ13ᵐ30ˢ.749
	// δ: -7°47′1″.74
}
Exemple #12
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func ExampleApproxPosition() {
	// Example 21.a, p. 132.
	eq := &coord.Equatorial{
		base.NewRA(10, 8, 22.3).Rad(),
		base.NewAngle(false, 11, 58, 2).Rad(),
	}
	epochFrom := 2000.0
	epochTo := 1978.0
	mα := base.NewHourAngle(true, 0, 0, 0.0169)
	mδ := base.NewAngle(false, 0, 0, 0.006)
	precess.ApproxPosition(eq, eq, epochFrom, epochTo, mα, mδ)
	fmt.Printf("%0.1d\n", base.NewFmtRA(eq.RA))
	fmt.Printf("%+0d\n", base.NewFmtAngle(eq.Dec))
	// Output:
	// 10ʰ07ᵐ12ˢ.1
	// +12°04′32″
}
Exemple #13
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func ExamplePosition() {
	// Example 21.b, p. 135.
	eq := &coord.Equatorial{
		base.NewRA(2, 44, 11.986).Rad(),
		base.NewAngle(false, 49, 13, 42.48).Rad(),
	}
	epochFrom := 2000.0
	jdTo := julian.CalendarGregorianToJD(2028, 11, 13.19)
	epochTo := base.JDEToJulianYear(jdTo)
	precess.Position(eq, eq, epochFrom, epochTo,
		base.NewHourAngle(false, 0, 0, 0.03425),
		base.NewAngle(true, 0, 0, 0.0895))
	fmt.Printf("%0.3d\n", base.NewFmtRA(eq.RA))
	fmt.Printf("%+0.2d\n", base.NewFmtAngle(eq.Dec))
	// Output:
	// 2ʰ46ᵐ11ˢ.331
	// +49°20′54″.54
}
Exemple #14
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func ExamplePosition() {
	// Example 33.a, p. 225.  VSOP87 result p. 227.
	earth, err := pp.LoadPlanet(pp.Earth, "")
	if err != nil {
		fmt.Println(err)
		return
	}
	venus, err := pp.LoadPlanet(pp.Venus, "")
	if err != nil {
		fmt.Println(err)
		return
	}
	α, δ := elliptic.Position(venus, earth, 2448976.5)
	fmt.Printf("α = %.3d\n", base.NewFmtRA(α))
	fmt.Printf("δ = %.2d\n", base.NewFmtAngle(δ))
	// Output:
	// α = 21ʰ4ᵐ41ˢ.454
	// δ = -18°53′16″.84
}