Chapter 19: Problem 35
A radiation of energy \(E\) falls normally on a perfectly absorbing surface. The momentum transferred to the surface is (A) \(\frac{E}{c}\) (B) \(\frac{2 E}{c}\) (C) \(E c\) (D) \(\frac{E}{c^{2}}\)
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Chapter 19: Problem 35
A radiation of energy \(E\) falls normally on a perfectly absorbing surface. The momentum transferred to the surface is (A) \(\frac{E}{c}\) (B) \(\frac{2 E}{c}\) (C) \(E c\) (D) \(\frac{E}{c^{2}}\)
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The energy that should be added to an electron, to reduce its de-Broglie wavelengths from \(10^{-10} \mathrm{~m}\) to \(0.5 \times 10^{-10} \mathrm{~m}\), will be (A) four times the initial energy. (B) thrice the initial energy. (C) equal to the initial energy. (D) twice the initial energy.
The electron in a hydrogen atom makes a transition \(n_{1} \rightarrow n_{2}\), where \(n_{1}\) and \(n_{2}\) are the principal quantum numbers of two states. Assume the Bohr model to be valid. If the time period of the electron in the initial state is eight times that in the final state then the possible values of \(n_{1}\) and \(n_{2}\) are (A) \(n_{1}=4, n_{2}=2\) (B) \(n_{1}=8, n_{2}=2\) (C) \(n_{1}=8, n_{2}=1\) (D) \(n_{1}=6, n_{2}=3\)
An alpha nucleus of energy \(\frac{1}{2} m v^{2}\) bombards a heavy nuclear target of charge \(\mathrm{Ze}\). Then the distance of closest approach for the alpha nucleus will be proportional to (A) \(v^{2}\) (B) \(\frac{1}{m}\) (C) \(\frac{1}{v^{2}}\) (D) \(\frac{1}{Z e}\)
Column-I represent the physical parameters being changed in the experiment of photo electric effect and in Column-II is its effect. Column-I (A) Intensity (B) Frequency (C) Potential difference between anode and cathode (D) Metal Column-II (1) photo electric current (2) stopping potential (3) work function (4) maximum kinetic energy
If the potential difference of Coolidge tube producing \(x\)-ray is increased, then choose the correct option(s). (A) the interval between \(\lambda_{k \alpha}\) and \(\lambda_{k \beta}\) increases (B) the interval between \(\lambda_{k \alpha}\) and \(\lambda_{0}\) increases (C) the interval between \(\lambda_{k \beta}\) and \(\lambda_{0}\) increases (D) \(\lambda_{0}\) does not change
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