Electromagnetic Waves
The mean intensity of radiation on the surface of the Sun is about $$10^8 \,W/m^2$$. The rms value of the corresponding magnetic field is closest to:
A light detector (your eye) has an area of $$2.00 \times 10^{-6} \mathrm{m}^{2}$$ and absorbs $$80 \%$$ of the incident light, which is at wavelength $$500 \mathrm{nm}$$. The detector faces an isotropic source, $$3.00 \mathrm{m}$$ from the source. If the detector absorbs photons at the rate of exactly $$4.000 \mathrm{s}^{-1},$$ at what power does the emitter emit light?
The rate at which photons are absorbed by the detector is related to the rate of photon emission by the light source via
$$R_{\mathrm{abs}}=(0.80) \dfrac{A_{\mathrm{abs}}}{4 \pi r^{2}} R_{\mathrm{emit}}\\$$
Given that $$A_{\text {bs }}=2.00 \times 10^{-6} \mathrm{m}^{2}$$ and $$r=3.00 \mathrm{m},$$ with $$R_{\text {abs }}=4.000$$ photons/s, we find the rate at which photons are emitted to be
$$R_{\text {emit }}=\dfrac{4 \pi r^{2}}{(0.80) A_{\text {abs }}} R_{\text {abs }}=\dfrac{4 \pi(3.00 \mathrm{m})^{2}}{(0.80)\left(2.00 \times 10^{-6} \mathrm{m}^{2}\right)}(4.000 \text { photons } / \mathrm{s})=2.83 \times 10^{8} \text { photons } / \mathrm{s}\\$$
since the energy of each emitted photon is
$$E_{\mathrm{ph}}=\dfrac{h c}{\lambda}=\dfrac{1240 \mathrm{eV} \cdot \mathrm{nm}}{500 \mathrm{nm}}=2.48 \mathrm{eV}\\$$
the power output of source is
$$P_{\mathrm{emit}}=R_{\mathrm{emit}} E_{\mathrm{ph}}=\left(2.83 \times 10^{8} \mathrm{photons} / \mathrm{s}\right)(2.48 \mathrm{eV})=7.0 \times 10^{8} \mathrm{eV} / \mathrm{s}=1.1 \times 10^{-10} \mathrm{W}\\$$
The mean intensity of radiation on the surface of the Sun is about $$10^8 \,W/m^2$$. The rms value of the corresponding magnetic field is closest to:
A block kept on a rough inclined plane, as shown in the figure, remains at rest upto a maximum force $$2 \,N$$ down the inclined plane. The maximum external force up the inclined plane that does not move the block is $$10 \,N$$. The coefficient of static friction between the block and the plane is : [Take $$g = 10 \,m/s^2$$]
The electric field in an electromagnetic wave is given by $$E=(100N/C)\sin\omega \left(t-\dfrac{x}{c}\right)$$ If the energy contained in a cylinder of cross-section $$10cm^3$$ and length $$50$$ cm along the x-axis is $$4.4\times 10^{-8} J/m^3$$, then the intensity of the wave is?
The average power per unit area at distance of $$2$$ m from a small bulb, if the bulb emits $$20$$W of electromagnetic radiation uniformly in all directions, will be?
A point isotropic sound source is located in the perpendicular to the plane of a ring drawn through the centre $$O$$ of the ring. The distance between the point $$O$$ and the source is $$l=1.00\ m$$ the radius of the ring is $$R=0.50\ m.$$ Find the mean energy flow across the area enclosed by the ring if at the point $$O$$ the intensity of sound is equal to $$I_{0}=30\mu\ W/m^{2}.$$ The damping of the waves is negligible.
The distance from the source at which the sound is not heard.
The wave intensity is defined by Eq. $$4.3i$$ $$I=\left(\Delta \right)^{2}_{m}/2\rho \nu$$
The oscillation amplitude of particles of the medium; compare it with the wavelength of sound.
A laser emits at 424 nm in a single pulse that lasts $$0.500 \mu s$$. The power of the pulse is 2.80MW. If we assume that the atoms contributing to the pulse underwent stimulated emission only once during the $$0.500 \mu s$$.how many atoms contributed?
In Figure, an isotropic point source of light S is positioned at distance d from a viewing screen A and the light intensity $$I_P$$ at point P (level with S) is measured. Then a plane mirror M is placed behind S at distance d. By how much is $$I_P$$ multiplied by the presence of the mirror?