In a plane EM wave, the electric field oscillates sinusoidally at a frequency of 5 times 10^10 mathrm~Hz and an amplitude of 50 mathrm~Vm^-1. The total average energy density of the electromagnetic field of the wave is : [Use varepsilon_0 = 8.85 times 10^-12 \, textC^2 / textNm^2 ]

Solution & Explanation

### Related Formula U_texttotal average = frac12epsilon_0 E_0^2 ### Core Logic For an electromagnetic wave, the total average energy density is the sum of the average energy density of the electric field and the magnetic field. They are equal, so: U_textavg = U_E + U_B = 2U_E = 2 left( frac14epsilon_0 E_0^2 right) = frac12epsilon_0 E_0^2 Where E_0 is the amplitude of the electric field. ### Step 2: Substitution Given: E_0 = 50 mathrm\, V/m epsilon_0 = 8.85 times 10^-12 mathrm\, C^2/(Ncdot m^2) U_textavg = frac12 times (8.85 times 10^-12) times (50)^2 U_textavg = frac12 times 8.85 times 10^-12 times 2500 U_textavg = 1.10625 times 10^-8 mathrm\, J/m^3 ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Waves

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More Electromagnetic Waves Previous-Year Questions — Page 4

Q46 jee_main_2024_27_jan_morning Energy Density and Intensity
A plane electromagnetic wave propagating in x-direction is described by E_y = (200text Vm^-1)sin[1.5 times 10^7t - 0.05x]. The intensity of the wave is (Use epsilon_0 = 8.85 times 10^-12text C^2textN^-1textm^-2):
  • A. 35.4text Wm^-2
  • B. 53.1text Wm^-2
  • C. 26.6text Wm^-2
  • D. 106.2text Wm^-2

Solution

### Related Formula I = frac12 epsilon_0 E_0^2 c Where E_0 is the amplitude of the electric field (200text V/m) and c = 3 times 10^8text m/s. ### Core Logic Substitute the constants into the equation: I = frac12 times (8.85 times 10^-12) times (200)^2 times (3 times 10^8) ### Step 1: Compute value I = frac12 times 8.85 times 10^-12 times 4 times 10^4 times 3 times 10^8 I = 2 times 8.85 times 3 times 10^0 I = 53.1text W/m^2 ### Pattern Recognition Isolate powers of ten first (10^-12 times 10^4 times 10^8 = 10^0) to streamline intermediate tracking accuracy on calculation variables. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Waves
Q40 jee_main_2024_29_jan_morning Maxwell Equations
Match List I with List II:
List IList II
A. oint vecB cdot dvecl = mu_0 i_c + mu_0 varepsilon_0 fracdphi_EdtI. Gauss' law for electricity
B. oint vecE cdot dvecl = -fracdphi_BdtII. Gauss' law for magnetism
C. oint vecE cdot dvecA = fracQvarepsilon_0III. Faraday law
D. oint vecB cdot dvecA = 0IV. Ampere - Maxwell law
Choose the correct answer from the options given below:
  • A. A-IV, B-I, C-III, D-II
  • B. A-II, B-III, C-I, D-IV
  • C. A-IV, B-III, C-I, D-II
  • D. A-I, B-II, C-III, D-IV

Solution

### Core Logic Let's review the fundamental Maxwell's equations: 1. **Ampere - Maxwell Law** relates the magnetic path integral to conduction current and displacement current: oint vecB cdot dvecl = mu_0 i_c + mu_0 varepsilon_0 fracdphi_Edt implies textA - IV 2. **Faraday's Law of Induction** states that changing magnetic flux induces an electromotive force (EMF): oint vecE cdot dvecl = -fracdphi_Bdt implies textB - III 3. **Gauss's Law for Electricity** relates net electric flux to enclosed charge: oint vecE cdot dvecA = fracQvarepsilon_0 implies textC - I 4. **Gauss's Law for Magnetism** states that magnetic monopoles do not exist: oint vecB cdot dvecA = 0 implies textD - II ### Step 1: Match Evaluation The match configurations are: * A rightarrow IV * B rightarrow III * C rightarrow I * D rightarrow II This perfectly corresponds to Option (3). ### Pattern Recognition Understand the integral geometries: Path integrals (line integrals oint cdot dvecl) correspond to circulating fields (induction laws like Ampere/Faraday). Surface integrals (flux integrals oint cdot dvecA) correspond to bounded charge states (Gauss laws). ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Waves Class 12 Physics: Electrostatics Class 12 Physics: Magnetism and Matter
Q40 jee_main_2024_30_january_evening Momentum of EM Waves
If the total energy transferred to a surface in time t is 6.48 times 10^5 mathrm~J, then the magnitude of the total momentum delivered to this surface for complete absorption will be:
  • A. 2.46 times 10^-3 mathrm~kg mathrm~m / mathrms
  • B. 2.16 times 10^-3 mathrm~kg mathrm~m / mathrms
  • C. 1.58 times 10^-3 mathrm~kg mathrm~m / mathrms
  • D. 4.32 times 10^-3 mathrm~kg mathrm~m / mathrms

Solution

### Related Formula p = fracUc ### Core Logic For an electromagnetic wave incident on a surface that is completely absorbed, the total momentum transferred is equal to the total energy transferred divided by the speed of light in vacuum (c). ### Step 1: Calculate Momentum Given total energy E = 6.48 times 10^5 mathrm~J. Speed of light c = 3 times 10^8 mathrm~m/s. p = fracEc = frac6.48 times 10^53 times 10^8 p = 2.16 times 10^-3 mathrm~kg~m/s ### Pattern Recognition Always check for "complete absorption" versus "perfect reflection". For complete absorption, p = E/c. For perfect reflection, p = 2E/c. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Waves
Q49 jee_main_2024_30_january_evening Maxwell's Equations
Match List I with List II:
List-IList-II
A. Gauss's law of magnetostaticsI. oint vecE cdot mathrmdveca = frac1varepsilon_0 int rho mathrmdV
B. Faraday's law of electro magnetic inductionII. oint vecB cdot mathrmdveca = 0
C. Ampere's lawIII. oint vecE cdot mathrmdvecl = -fracmathrmdmathrmdtint vecB cdot mathrmdveca
D. Gauss's law of electrostaticsIV. oint vecB cdot mathrmdvecl = mu_0 I
Choose the correct answer from the options given below:
  • A. textA-I, B-III, C-IV, D-II
  • B. textA-III, B-IV, C-I, D-II
  • C. textA-IV, B-II, C-III, D-I
  • D. textA-II, B-III, C-IV, D-I

Solution

### Core Logic Match each law with its corresponding mathematical expression (Maxwell's equations). (A) Gauss's law of magnetostatics: The net magnetic flux through any closed surface is zero. oint vecB cdot mathrmdveca = 0 (Matches II). (B) Faraday's law of electromagnetic induction: The induced electromotive force in any closed circuit is equal to the negative of the time rate of change of the magnetic flux. oint vecE cdot mathrmdvecl = -fracmathrmdmathrmdt int vecB cdot mathrmdveca (Matches III). (C) Ampere's law: The line integral of the magnetic field around a closed loop is proportional to the electric current passing through the loop. oint vecB cdot mathrmdvecl = mu_0 I (Matches IV). (D) Gauss's law of electrostatics: The electric flux through any closed surface is proportional to the enclosed electric charge. oint vecE cdot mathrmdveca = frac1varepsilon_0 int rho mathrmdV (Matches I). ### Step 1: Final Match A rightarrow II B rightarrow III C rightarrow IV D rightarrow I This matches option (4). ### Pattern Recognition These are the fundamental Maxwell equations in integral form. Memorizing their direct mappings guarantees quick marks. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Waves Class 12 Physics: Electromagnetic Induction
Q38 jee_main_2024_30_jan_morning Properties of EM Waves
The electric field of an electromagnetic wave in free space is represented as vecE = E_0cos (omega t - kz)hati The corresponding magnetic induction vector will be:
  • A. vecB = E_0Ccos (omega t - kz)hatj
  • B. vecB = fracE_0C cos (omega t - kz) hatj
  • C. vecB = E_0Ccos (omega t + kz)hatj
  • D. vecB = fracE_0Ccos (omega t + kz)hatj

Solution

### Related Formula B_0 = fracE_0C hatC = hatE times hatB ### Core Logic In an electromagnetic wave in free space, the magnitudes of the electric and magnetic fields are related by E_0 = c B_0. Thus, B_0 = E_0 / C. The direction of wave propagation is given by the cross product of the electric field and magnetic field vectors: hatC = hatE times hatB. ### Step 1: Determine Wave Direction and Magnetic Field Direction Given the phase term (omega t - kz), the wave propagates in the +z direction, so hatC = hatk. The electric field oscillates in the +x direction, so hatE = hati. We know: hatk = hati times hatB Since hati times hatj = hatk, the magnetic field must oscillate in the +y direction (hatj). ### Step 2: Construct Final Vector The full magnetic field vector shares the same phase and applies the above amplitude and direction: vecB = fracE_0C cos(omega t - kz) hatj ### Pattern Recognition Phase remains identical. Amplitude scales by 1/c. Direction satisfies the right-hand triad (vecE, vecB, vecv) where vecv = vecE times vecB. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Waves

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