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topjm [15]
4 years ago
10

In a double slit experiment, if the separation between the two slits is 0.050 mm and the distance from the slits to a screen is

2.5 m, find the spacing between the first-order and second-order bright fringes when coherent light of wavelength 600 nm illuminates the slits.
Physics
1 answer:
Lera25 [3.4K]4 years ago
8 0

Answer:

30 cm

Explanation:

Hi! Lets find the angles for the first and second order maxima

The first order maximum will occur for Ф=0

The second order maximum will satisfy the following relationship:

sinФ = λ/d

Where   λ = 600 x 10^-9 m  and d = 5 x 10^-5 m

Therefore:

sinФ = 0.012

And the vertical distance bewteen the first and second will be given by:

l = (2.5 m) tanФ

But since 2.5 m>>0.05 mm  ;  sinФ≈tanФ

Therefore:

l = (2.5 m) sinФ

l = 0.03 m = 30 cm

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Answer:

Approximately 1.44\times 10^3 \; \rm N \cdot m^{-1} assuming that the spring has zero mass.

Explanation:

Without any external force, a piece of mass connected to an ideal spring (like the chair in this question) will undergo simple harmonic oscillation.

On the other hand, the force constant of a spring (i.e., its stiffness) can be found using Hooke's Law. If the spring exerts a restoring force \mathbf{F} when its displacement is \mathbf{x}, then its force constant would be:

\displaystyle k = -\frac{\mathbf{F}}{\mathbf{x}}.  

The goal here is to find the expressions for F and for x. By Hooke's Law, the spring constant would be ratio of these two expressions.

Let T represent the time period of this oscillation. With the chair alone, the period of oscillation is T = 1.00\; \rm s.

For a simple harmonic oscillation, the angular frequency \omega can be found from the period:

\displaystyle \omega = \frac{2\pi}{T}.

Let A stands for the amplitude of this oscillation. In a simple harmonic oscillation, both \mathbf{F} and \mathbf{x} are proportional to A. Keep in mind that the spring constant k is simply the opposite of the ratio between \mathbf{F} and \mathbf{x}. Therefore, the exact value of A shouldn't really affect the value of the spring constant.

In a simple harmonic motion (one that starts with maximum displacement and zero velocity,) the displacement (from equilibrium position) at time t would be:

\displaystyle \mathbf{x}(t) = A \cos(\omega \cdot t).

The restoring velocity at time t would be:

\displaystyle \mathbf{v}(t) = \mathbf{x}^\prime(t) = -A\, \omega \sin(\omega\cdot t).

The restoring acceleration at time t would be:

\displaystyle \mathbf{a}(t) = \mathbf{v}^\prime(t) = -A\, \omega^2 \cos(\omega\cdot t).

Assume that the spring has zero mass. By Newton's Second Law of motion, the restoring force at time t would be:

\begin{aligned}& \mathbf{F}(t) \\ &= m(\text{chair}) \cdot \mathbf{a}(t) \\&= -m(\text{chair}) \, A\, \omega^2 \cos(\omega \cdot t)\end{aligned}.

Apply Hooke's Law to find the spring constant, k:

\begin{aligned} k & = -\frac{\mathbf{F}}{\mathbf{x}} \\ &= -\left(\frac{-m(\text{chair}) \, A\, \omega^2 \cos(\omega \cdot t)}{A\cos(\omega \cdot t)}\right) \\ &= \omega^2 \cdot  m(\text{chair}) \end{aligned}.

Again, \omega stands for the angular frequency of this oscillation, where

\displaystyle \omega = \frac{2\pi}{T}.

Before proceeding, note how A was eliminated from the ratio (as expected.) Additionally, t is also eliminated from the ratio. In other words, the spring constant is "constant" at all time. That agrees with the assumption that this spring is indeed ideal. Back to k:

\begin{aligned} k & = -\frac{\mathbf{F}}{\mathbf{x}} \\ &= \cdots \\ &= \omega^2 \cdot  m(\text{chair}) \\ &= \left(\frac{2\pi}{T}\right)^2 \cdot m(\text{chair}) \\ &= \left(\frac{2\pi}{1.00\; \rm s}\right)^2 \times 36.4\; \rm kg\end{aligned}.

Side note on the unit of k:

\begin{aligned} & 1\; \rm kg \cdot s^{-2} \\ &= 1\rm \; \left(kg \cdot m \cdot s^{-2}\right) \cdot m^{-1} \\ &= 1\; \rm N \cdot m^{-1}\end{aligned}.

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A uniformly charged rod of length L = 1.3 m lies along the x-axis with its right end at the origin. The rod has a total charge o
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Answer:

E = 3544.44 N/C

Explanation:

Given:

- charge Q = 2.2 *10^-6 C

- Length L = 1.3 m

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Solution:

- The differential electric field dE due to infinitesimal charge dq can be considered as a point charge at a distance of r is given by:

                                  dE = k*dq / r^2

- The charge Q is spread over entire length L, hence:

                                  dq = (Q / L ) * dx

-The resulting dE:

                                 dE = (k*Q/L)*(dx / r^2)

- point P lies on the x- axis with distance (x+a) from differential charge from:

                                 dE = (k*Q/L)*(dx / (x+a)^2)  

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                                 E =  (-k*Q/L)* (1 / a - 1 / (L+a))

                                 E =  (-k*Q/L)* (L / a(L+a))

                                 E = (k*Q / a(L+a))

- Evaluate E @ a = 1.8 m

                                 E =(8.99*10^9 * 2.2*10^-6 / 1.8*(1.3+1.8))

                                 E = 3544.44 N/C

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