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14.3: Intensity in Single-Slit Diffraction
https://phys.libretexts.org/Courses/Muhlenberg_College/Physics_122%3A_General_Physics_II_(Collett)/14%3A_Diffraction/14.03%3A_Intensity_in_Single-Slit_Diffraction
The intensity pattern for diffraction due to a single slit can be calculated using phasors as $I = I_0 \left(\frac{sin \space \beta}{\beta}\right)^2,$ where \(\beta = \frac{\phi}{2} = \frac{\pi D \...The intensity pattern for diffraction due to a single slit can be calculated using phasors as $I = I_0 \left(\frac{sin \space \beta}{\beta}\right)^2,$ where $\beta = \frac{\phi}{2} = \frac{\pi D \space sin \space \theta}{\lambda}$ , D is the slit width, λλ is the wavelength, and θθ is the angle from the central peak.
1.7: Notation
https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/01%3A_Preliminary_Concepts/1.07%3A_Notation
The list below describes notation used in this book
4.3: Intensity in Single-Slit Diffraction
https://phys.libretexts.org/Courses/Bowdoin_College/Phys1140%3A_Introductory_Physics_II%3A_Part_2/04%3A_Diffraction/4.03%3A_Intensity_in_Single-Slit_Diffraction
The intensity pattern for diffraction due to a single slit can be calculated using phasors as $I = I_0 \left(\frac{sin \space \beta}{\beta}\right)^2,$ where \(\beta = \frac{\phi}{2} = \frac{\pi D \...The intensity pattern for diffraction due to a single slit can be calculated using phasors as $I = I_0 \left(\frac{sin \space \beta}{\beta}\right)^2,$ where $\beta = \frac{\phi}{2} = \frac{\pi D \space sin \space \theta}{\lambda}$ , D is the slit width, λλ is the wavelength, and θθ is the angle from the central peak.
1.7: Notation
https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_I_(Ellingson)/01%3A_Preliminary_Concepts/1.07%3A_Notation
The list below describes notation used in this book
1.6: Notation
https://phys.libretexts.org/Courses/Kettering_University/Electricity_and_Magnetism_with_Applications_to_Amateur_Radio_and_Wireless_Technology/01%3A_Preliminary_Concepts/1.06%3A_Notation
The section summarizes the notation used in this book.
4.3: Intensity in Single-Slit Diffraction
https://phys.libretexts.org/Bookshelves/University_Physics/University_Physics_(OpenStax)/University_Physics_III_-_Optics_and_Modern_Physics_(OpenStax)/04%3A_Diffraction/4.03%3A_Intensity_in_Single-Slit_Diffraction
The intensity pattern for diffraction due to a single slit can be calculated using phasors as $I = I_0 \left(\frac{sin \space \beta}{\beta}\right)^2,$ where \(\beta = \frac{\phi}{2} = \frac{\pi D \...The intensity pattern for diffraction due to a single slit can be calculated using phasors as $I = I_0 \left(\frac{sin \space \beta}{\beta}\right)^2,$ where $\beta = \frac{\phi}{2} = \frac{\pi D \space sin \space \theta}{\lambda}$ , D is the slit width, λλ is the wavelength, and θθ is the angle from the central peak.
21.2: Phasors
https://phys.libretexts.org/Courses/Kettering_University/Electricity_and_Magnetism_with_Applications_to_Amateur_Radio_and_Wireless_Technology/21%3A_Electrical_Transmission_Lines/21.02%3A_Phasors
In many areas of engineering, signals are well-modeled as sinusoids. Also, devices that process these signals are often well-modeled as linear time-invariant (LTI) systems. The response of an LTI syst...In many areas of engineering, signals are well-modeled as sinusoids. Also, devices that process these signals are often well-modeled as linear time-invariant (LTI) systems. The response of an LTI system to any linear combination of sinusoids is another linear combination of sinusoids having the same frequencies.
9.2: Phasors
https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Book%3A_Applications_of_Maxwells_Equations_(Cochran_and_Heinrich)/09%3A_Plane_Waves_I/9.02%3A_Phasors
It is very convenient to represent sinusoidal functions i.e. sines and cosines, by complex exponential functions when dealing with linear differential equations such as Maxwell’s equations.
1.5: Phasors
https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_I_(Ellingson)/01%3A_Preliminary_Concepts/1.05%3A_Phasors
In many areas of engineering, signals are well-modeled as sinusoids. Also, devices that process these signals are often well-modeled as linear time-invariant (LTI) systems. The response of an LTI syst...In many areas of engineering, signals are well-modeled as sinusoids. Also, devices that process these signals are often well-modeled as linear time-invariant (LTI) systems. The response of an LTI system to any linear combination of sinusoids is another linear combination of sinusoids having the same frequencies.
22.2: AC Circuits
https://phys.libretexts.org/Bookshelves/University_Physics/Physics_(Boundless)/22%3A_Induction_AC_Circuits_and_Electrical_Technologies/22.2%3A_AC_Circuits
Induction is the process in which an emf is induced by changing magnetic flux, such as a change in the current of a conductor.
1.5: Phasors
https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/01%3A_Preliminary_Concepts/1.05%3A_Phasors
In many areas of engineering, signals are well-modeled as sinusoids. Also, devices that process these signals are often well-modeled as linear time-invariant (LTI) systems. The response of an LTI syst...In many areas of engineering, signals are well-modeled as sinusoids. Also, devices that process these signals are often well-modeled as linear time-invariant (LTI) systems. The response of an LTI system to any linear combination of sinusoids is another linear combination of sinusoids having the same frequencies.

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