Lösningsförslag till typuppgifter optik - Versionshistorik

Hakan: /* Interferens i dubbelspalt */

2015-03-08T12:48:30Z

Interferens i dubbelspalt

← Äldre version		Versionen från 8 mars 2015 kl. 12.48
Rad 55:		Rad 55:

	[[Image:Single slit and double slit2.jpg\|right\|350px\|thumb\|Same double-slit assembly (0.7mm between slits); in top image, one slit is closed. In the single-slit image, a [[diffraction pattern]] (the faint spots on either side of the main band) forms due to the nonzero width of the slit. A diffraction pattern is also seen in the double-slit image, but at twice the intensity and with the addition of many smaller interference fringes.]]		[[Image:Single slit and double slit2.jpg\|right\|350px\|thumb\|Same double-slit assembly (0.7mm between slits); in top image, one slit is closed. In the single-slit image, a [[diffraction pattern]] (the faint spots on either side of the main band) forms due to the nonzero width of the slit. A diffraction pattern is also seen in the double-slit image, but at twice the intensity and with the addition of many smaller interference fringes.]]
	: <math> tan \alpha _n = \frac{x_n}{l} </math>
			: <math> tan \: \alpha _n = \frac{x_n}{l} </math>

2015-03-08T12:48:00Z

Interferens i dubbelspalt

← Äldre version		Versionen från 8 mars 2015 kl. 12.48
Rad 60:		Rad 60:
	[[File:Double-slit.PNG\|thumb\|Photons or particles of matter (like an electron) produce a wave pattern when two slits are used]]		[[File:Double-slit.PNG\|thumb\|Photons or particles of matter (like an electron) produce a wave pattern when two slits are used]]

	: <math> sin \alpha _n = \frac{n \lambda}{d} </math>		: <math> sin \: \alpha _n = \frac{n \lambda}{d} </math>

	{{enwp\|Double-slit_experiment}}		{{enwp\|Double-slit_experiment}}

2015-03-08T12:47:02Z

Totalreflektion

← Äldre version		Versionen från 8 mars 2015 kl. 12.47
Rad 17:		Rad 17:
	Ljus genom det tätare mediet reflekteras i ytan mot det tunnare mediet. Om det är luft fås :		Ljus genom det tätare mediet reflekteras i ytan mot det tunnare mediet. Om det är luft fås :

	: <math> n_1 \cdot sin v_1 = 1.00 \cdot sin 90^o </math>		: <math> n_1 \cdot sin \: v_1 = 1.00 \cdot sin \: 90^o </math>

	eller helt enkelt:		eller helt enkelt:

	: <math> n_1 \cdot sin v_1 = 1 </math>		: <math> n_1 \cdot sin \: v_1 = 1 </math>

	=== Räkna ===		=== Räkna ===

2015-03-08T12:46:18Z

Brytningslagen

← Äldre version		Versionen från 8 mars 2015 kl. 12.46
Rad 2:		Rad 2:
	{{Heureka2 \|191}}		{{Heureka2 \|191}}

	: <math> n_1 \cdot sin v_1 = n_2 \cdot sin v_2 </math>		: <math> n_1 \cdot sin \: v_1 = n_2 \cdot sin \: v_2 </math>

	=== Räkna ===		=== Räkna ===

2015-03-06T12:22:00Z

Newtons avbildningsformel

← Äldre version		Versionen från 6 mars 2015 kl. 12.22
Rad 30:		Rad 30:

	{{Heureka2 \|199}}		{{Heureka2 \|199}}
			Uppg: 10.17-10.21

	Lada ner den [http://tube.geogebra.org/student/m15141 här] GGB och lägg in sträckorna till formeln:		Lada ner den [http://tube.geogebra.org/student/m15141 här] GGB och lägg in sträckorna till formeln:

2015-03-06T12:04:22Z

Interferens i dubbelspalt

← Äldre version		Versionen från 6 mars 2015 kl. 12.04
Rad 50:		Rad 50:

	{{heureka2\|215}}		{{heureka2\|215}}

			Räkna 11.4-11.7

	[[Image:Single slit and double slit2.jpg\|right\|350px\|thumb\|Same double-slit assembly (0.7mm between slits); in top image, one slit is closed. In the single-slit image, a [[diffraction pattern]] (the faint spots on either side of the main band) forms due to the nonzero width of the slit. A diffraction pattern is also seen in the double-slit image, but at twice the intensity and with the addition of many smaller interference fringes.]]		[[Image:Single slit and double slit2.jpg\|right\|350px\|thumb\|Same double-slit assembly (0.7mm between slits); in top image, one slit is closed. In the single-slit image, a [[diffraction pattern]] (the faint spots on either side of the main band) forms due to the nonzero width of the slit. A diffraction pattern is also seen in the double-slit image, but at twice the intensity and with the addition of many smaller interference fringes.]]

2015-03-06T12:03:20Z

Interferens i dubbelspalt

2015-03-06T12:02:46Z

Interferens i dubbelspalt

← Äldre version		Versionen från 6 mars 2015 kl. 12.02
Rad 51:		Rad 51:
	{{heureka2\|215}}		{{heureka2\|215}}

			[[Image:Single slit and double slit2.jpg\|right\|350px\|thumb\|Same double-slit assembly (0.7mm between slits); in top image, one slit is closed. In the single-slit image, a [[diffraction pattern]] (the faint spots on either side of the main band) forms due to the nonzero width of the slit. A diffraction pattern is also seen in the double-slit image, but at twice the intensity and with the addition of many smaller interference fringes.]]
	: <math> tan \alpha _n = \frac{x_n}{l} </math>		: <math> tan \alpha _n = \frac{x_n}{l} </math>


			[[File:Double-slit.PNG\|thumb\|Photons or particles of matter (like an electron) produce a wave pattern when two slits are used]]

	: <math> sin \alpha _n = \frac{n \lambda}{d} </math>		: <math> sin \alpha _n = \frac{n \lambda}{d} </math>

2015-03-06T12:01:28Z

Interferens i dubbelspalt

← Äldre version		Versionen från 6 mars 2015 kl. 12.01
Rad 54:		Rad 54:

	: <math> sin \alpha _n = \frac{n \lambda}{d} </math>		: <math> sin \alpha _n = \frac{n \lambda}{d} </math>

			{{enwp\|Double-slit_experiment}}

	== Gitter ==		== Gitter ==

2015-03-05T23:03:36Z

Gitter

← Äldre version		Versionen från 5 mars 2015 kl. 23.03
Rad 59:		Rad 59:
	{{heureka2\|217}}		{{heureka2\|217}}

	: <math> n \lambda = d \: \sin \alpha_n} </math>		: <math> n \: \lambda = d \: \sin \: \alpha_n} </math>