The number of bright interference fringes in the central diffraction maximum can be found using the formula:
n = (d sin θ) / λwhere n is the number of fringes, d is the distance between the slits, θ is the angle between the central maximum and the first bright fringe, and λ is the wavelength of light.
For the central maximum, the angle θ is zero, so sin θ = 0. Therefore, the equation simplifies to:
n = 0So there are no bright interference fringes in the central diffraction maximum.
The number of bright interference fringes in the whole pattern can be found using the formula:
n = (mλD) / dwhere n is the number of fringes, m is the order of the fringe, λ is the wavelength of light, D is the distance from the slits to the screen, and d is the distance between the slits.
To find the maximum value of m, we can use the condition for constructive interference:
d sin θ = mλwhere θ is the angle between the direction of the fringe and the direction of the center of the pattern.
For the first bright fringe on either side of the central maximum, sin θ = λ/d. Therefore, the value of m for the first bright fringe is:
m = d/λSubstituting this value of m into the formula for the number of fringes, we get:
n = (d/λ)(λD/d) = DSo there are D bright interference fringes in the whole pattern, where D is the distance from the slits to the screen, in units of the wavelength of light.
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Consider three identical metal spheres, a, b, and c. sphere a carries a charge of 5q. sphere b carries a charge of -q. sphere c carries no net charge. spheres a and b are touched together and then separated. sphere c is then touched to sphere a and separated from it. lastly, sphere c is touched to sphere b and separated from it.
required:
a. how much charge ends up on sphere c?
b. what is the total charge on the three spheres before they are allowed to touch each other?
a. Sphere c ends up with a charge of -3q.
b. The total charge on the three spheres before they are allowed to touch each other is 5q - q = 4q.
a. When spheres a and b are touched together and then separated, charge is transferred between them until they reach equilibrium. Since sphere a has a charge of 5q and sphere b has a charge of -q, the total charge transferred is 5q - (-q) = 6q. This charge is shared equally between the two spheres, so sphere a ends up with a charge of 5q - 3q = 2q, and sphere b ends up with a charge of -q + 3q = 2q.
When sphere c is touched to sphere a and separated, they share charge. Sphere a has a charge of 2q, and sphere c has no net charge initially. The charge is shared equally, so both spheres end up with a charge of q.
Similarly, when sphere c is touched to sphere b and separated, they also share charge. Sphere b has a charge of 2q, and sphere c has a charge of q. The charge is shared equally, so both spheres end up with a charge of (2q + q) / 2 = 3q/2.
Therefore, sphere c ends up with a charge of -3q (opposite sign due to excess electrons) and the total charge on the three spheres before they are allowed to touch each other is 5q - q = 4q.
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Calculate the angular separation of two Sodium lines given as 580.0nm and 590.0 nm in first order spectrum. Take the number of ruled lines per unit length on the diffraction grating as 300 per mm?
(A) 0.0180
(B) 180
(C) 1.80
(D) 0.180
The angular separation of two Sodium lines is calculated as (C) 1.80.
The angular separation between the two Sodium lines can be calculated using the formula:
Δθ = λ/d
Where Δθ is the angular separation, λ is the wavelength difference between the two lines, and d is the distance between the adjacent ruled lines on the diffraction grating.
First, we need to convert the given wavelengths from nanometers to meters:
λ1 = 580.0 nm = 5.80 × 10⁻⁷ m
λ2 = 590.0 nm = 5.90 × 10⁻⁷ m
The wavelength difference is:
Δλ = λ₂ - λ₁ = 5.90 × 10⁻⁷ m - 5.80 × 10⁻⁷ m = 1.0 × 10⁻⁸ m
The distance between adjacent ruled lines on the diffraction grating is given as 300 lines per mm, which can be converted to lines per meter:
d = 300 lines/mm × 1 mm/1000 lines × 1 m/1000 mm = 3 × 10⁻⁴ m/line
Substituting the values into the formula, we get:
Δθ = Δλ/d = (1.0 × 10⁻⁸ m)/(3 × 10⁻⁴ m/line) = 0.033 radians
Finally, we convert the answer to degrees by multiplying by 180/π:
Δθ = 0.033 × 180/π = 1.89 degrees
Rounding off to two significant figures, the answer is:
(C) 1.80
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