In an interference arrangement similar to Young's double slit experiment, the slits S, and S, are illuminated with coherent microwave sources each of frequency 106 Hz. The sources are synchronized to have zero phase difference. The slits are separated by distance d = 150 m. The intensity (0) is measured as a function of o, where 0 is defined as shown. If I, is maximum intensity, then (0) for 0

In an interference arrangement similar to Young's double-slit experiment, the slits S_1 and S_2 are illuminated with coherent microwave sources, each of frequency 10^6 Hz. The sources are synchronized to have zero phase difference. The slits are separated by a distance d=150.0 m. The intensity I (theta) is measured as a function of theta, where theta is defined as shown. If I_0 is the maximum intensity, then I (theta) for 0lethetale90degree is given by

In an interference arrangement similar to Young's double-slit experiment, the slits S_1 and S_2 are illuminated with coherent microwave sources, each of frequency 10^6 Hz. The sources are synchronized to have zero phase difference. The slits are separated by a distance d=150.0 m. The intensity I (theta) is measured as a function of theta, where theta is defined as shown. If I_0 is the maximum intensity, then I (theta) for 0lethetale90degree is given by

In an interference arrangement similar to young's double slit experiment the slits S_(1) and S_(2) are illuminated with coherent microwave sources each of frequency 10^(6)Hz the sources are synchronized to have zero phase difference. the slits are separated by a distance d=150.0m. The intensity I(theta) is measured as a funtion of theta , where theta is defined as shown. if I_(0) is the maximum intensity then I(theta) for 0lethetale90^(@) is given by:

In an interference arrangement similar to young's double slit experiment the slits S_(1) and S_(2) are illuminated with coherent microwave sources each of frequency 10^(6)Hz the sources are synchronized to have zero phase difference. the slits are separated by a distance d=150.0m. The intensity I(theta) is measured as a funtion of theta , where theta is defined as shown. if I_(0) is the maximum intensity then I(theta) for 0lethetale90^(@) is given by:

In an interference arrangement similar to double-slit experiment, S_(1) and S_(2) are illuminated with coherent source microwave source each of frequency 1 MHz. the sources are synchronized to have zero phase difference . This slits are separated by distance d = 150.0m The intensity I (theta) is measured as a funciton of theta , where theta is defined as shown in figure. If I_(0) is maximum intensity, calculate I (theta) For : a. theta = 0 b. theta = 30^(@) c. theta = 90^(@)

Consider an interference arrangement similar to YDSE. Slits S_(1) and S_(2) are illuminated with coherent microwave sources each of frequency 2 MHz The sources are synchronized to have zero phase difference. The slits are separated by distance d= 75m. The intensity I_((theta)) is measured as a function of theta where theta is defined as shown in figure. if I_(0) is maximum intensity then calculated I_((theta)) for (i) theta= 0^(@), (ii) theta=pi//6 and (iii) theta = pi//2

Consider an interference arrangement similar to YDSE. Slits S_(1) and S_(2) are illuminated with coherent microwave sources each of frequency 2 MHz. The sources are synchronised to have zero phase difference. The slits are separated by distance d= 75m. The intensity I_((theta)) is measured as a function of theta where theta is defined as shown in figure. if I_(0) is maximum intensity then calculated I_((theta)) for (i) theta= 0^(@), (ii) theta=pi//6 and (iii) theta = pi//2