X-Rays Electromagnetic Radiation, Moseley law, Internal Structure Of Matter
Dual nature of radiation and Matter

142653 X-ray of wavelength \(\lambda=2 \AA\) is emitted from the metal target. The potential difference applied across the cathode and the metal target is

1 \(5525 \mathrm{~V}\)
2 \(320 \mathrm{~V}\)
3 \(6200 \mathrm{~V}\)
4 \(3250 \mathrm{~V}\)
Dual nature of radiation and Matter

142589 Which of the following wavelengths falls in Xray region?

1 \(10000 \mathrm{~A}\)
2 \(1000 \mathrm{~A}\)
3 \(1 \mathrm{~A}\)
4 \(10^{-2} \AA\)
Dual nature of radiation and Matter

142592 If \(\mathrm{V}\) be the aceelerating voltage of the tube, the maximum frequency of continuous x-rays produced depends on \(V\) as

1 \(V^2\)
2 \(\mathrm{V}\)
3 \(\mathrm{V}^{1 / 2}\)
4 \(\mathrm{V}^{-1}\)
Dual nature of radiation and Matter

142596 The potential difference applied to an \(X\)-ray tube is \(5 \mathrm{kV}\) and the current through it is \(\mathbf{3 . 2}\) \(\mathrm{mA}\). Then the number of electrons striking the target per second is

1 \(5 \times 10^6\)
2 \(2 \times 10^{16}\)
3 \(1 \times 10^{17}\)
4 \(4 \times 10^{18}\)
Dual nature of radiation and Matter

142653 X-ray of wavelength \(\lambda=2 \AA\) is emitted from the metal target. The potential difference applied across the cathode and the metal target is

1 \(5525 \mathrm{~V}\)
2 \(320 \mathrm{~V}\)
3 \(6200 \mathrm{~V}\)
4 \(3250 \mathrm{~V}\)
Dual nature of radiation and Matter

142589 Which of the following wavelengths falls in Xray region?

1 \(10000 \mathrm{~A}\)
2 \(1000 \mathrm{~A}\)
3 \(1 \mathrm{~A}\)
4 \(10^{-2} \AA\)
Dual nature of radiation and Matter

142592 If \(\mathrm{V}\) be the aceelerating voltage of the tube, the maximum frequency of continuous x-rays produced depends on \(V\) as

1 \(V^2\)
2 \(\mathrm{V}\)
3 \(\mathrm{V}^{1 / 2}\)
4 \(\mathrm{V}^{-1}\)
Dual nature of radiation and Matter

142596 The potential difference applied to an \(X\)-ray tube is \(5 \mathrm{kV}\) and the current through it is \(\mathbf{3 . 2}\) \(\mathrm{mA}\). Then the number of electrons striking the target per second is

1 \(5 \times 10^6\)
2 \(2 \times 10^{16}\)
3 \(1 \times 10^{17}\)
4 \(4 \times 10^{18}\)
Dual nature of radiation and Matter

142653 X-ray of wavelength \(\lambda=2 \AA\) is emitted from the metal target. The potential difference applied across the cathode and the metal target is

1 \(5525 \mathrm{~V}\)
2 \(320 \mathrm{~V}\)
3 \(6200 \mathrm{~V}\)
4 \(3250 \mathrm{~V}\)
Dual nature of radiation and Matter

142589 Which of the following wavelengths falls in Xray region?

1 \(10000 \mathrm{~A}\)
2 \(1000 \mathrm{~A}\)
3 \(1 \mathrm{~A}\)
4 \(10^{-2} \AA\)
Dual nature of radiation and Matter

142592 If \(\mathrm{V}\) be the aceelerating voltage of the tube, the maximum frequency of continuous x-rays produced depends on \(V\) as

1 \(V^2\)
2 \(\mathrm{V}\)
3 \(\mathrm{V}^{1 / 2}\)
4 \(\mathrm{V}^{-1}\)
Dual nature of radiation and Matter

142596 The potential difference applied to an \(X\)-ray tube is \(5 \mathrm{kV}\) and the current through it is \(\mathbf{3 . 2}\) \(\mathrm{mA}\). Then the number of electrons striking the target per second is

1 \(5 \times 10^6\)
2 \(2 \times 10^{16}\)
3 \(1 \times 10^{17}\)
4 \(4 \times 10^{18}\)
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Dual nature of radiation and Matter

142653 X-ray of wavelength \(\lambda=2 \AA\) is emitted from the metal target. The potential difference applied across the cathode and the metal target is

1 \(5525 \mathrm{~V}\)
2 \(320 \mathrm{~V}\)
3 \(6200 \mathrm{~V}\)
4 \(3250 \mathrm{~V}\)
Dual nature of radiation and Matter

142589 Which of the following wavelengths falls in Xray region?

1 \(10000 \mathrm{~A}\)
2 \(1000 \mathrm{~A}\)
3 \(1 \mathrm{~A}\)
4 \(10^{-2} \AA\)
Dual nature of radiation and Matter

142592 If \(\mathrm{V}\) be the aceelerating voltage of the tube, the maximum frequency of continuous x-rays produced depends on \(V\) as

1 \(V^2\)
2 \(\mathrm{V}\)
3 \(\mathrm{V}^{1 / 2}\)
4 \(\mathrm{V}^{-1}\)
Dual nature of radiation and Matter

142596 The potential difference applied to an \(X\)-ray tube is \(5 \mathrm{kV}\) and the current through it is \(\mathbf{3 . 2}\) \(\mathrm{mA}\). Then the number of electrons striking the target per second is

1 \(5 \times 10^6\)
2 \(2 \times 10^{16}\)
3 \(1 \times 10^{17}\)
4 \(4 \times 10^{18}\)