Wave Nature of Matter
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357896 Nuclear radii may be measured by scattering high energy electrons from nuclei. What is the de-Broglie wavelength for \(200\,M{\mkern 1mu} eV\) electrons?

1 \(8.28\,Fm\)
2 \(7.98\,Fm\)
3 \(6.45\,Fm\)
4 \(6.20\,Fm\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357897 An electron is accelerated from rest through a potential difference of \(\) volt. If the de Broglie wavelength of the electron is \(1.227 \times {10^{ - 2}}\;nm\), the potential difference is:

1 \({10^2}\;V\)
2 \({10^3}\;V\)
3 \({10^4}\;V\)
4 \(10\;V\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357898 A particle \({P}\) is formed due to a completely inelastic collision of particles \({x}\) and \({y}\), having de-Broglie wavelengths \({\lambda_{x}}\) and \({\lambda_{y}}\) respectively. If \({x}\) and \({y}\) were moving in opposite directions, then the de Broglie wavelength of \({p}\) is

1 \({\lambda_{x}+\lambda_{y}}\)
2 \({\dfrac{\lambda_{x} \lambda_{y}}{\lambda_{x}+\lambda_{y}}}\)
3 \({\dfrac{\lambda_{x} \lambda_{y}}{\left|\lambda_{x}-\lambda_{y}\right|}}\)
4 \({\lambda_{x}-\lambda_{y}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357899 When a proton is accelerated with 1 volt potential difference, its kinetic energy is

1 1840 \(eV\)
2 1 \(eV\)
3 184 \(eV\)
4 18400 \(eV\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357900 A particle is dropped from a height ' \(H\) '. The de Broglie wavelength of the particle depends on height as

1 \(H\)
2 \({H^{ - 1/2}}\)
3 \({H^0}\)
4 \({H^{1/2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357896 Nuclear radii may be measured by scattering high energy electrons from nuclei. What is the de-Broglie wavelength for \(200\,M{\mkern 1mu} eV\) electrons?

1 \(8.28\,Fm\)
2 \(7.98\,Fm\)
3 \(6.45\,Fm\)
4 \(6.20\,Fm\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357897 An electron is accelerated from rest through a potential difference of \(\) volt. If the de Broglie wavelength of the electron is \(1.227 \times {10^{ - 2}}\;nm\), the potential difference is:

1 \({10^2}\;V\)
2 \({10^3}\;V\)
3 \({10^4}\;V\)
4 \(10\;V\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357898 A particle \({P}\) is formed due to a completely inelastic collision of particles \({x}\) and \({y}\), having de-Broglie wavelengths \({\lambda_{x}}\) and \({\lambda_{y}}\) respectively. If \({x}\) and \({y}\) were moving in opposite directions, then the de Broglie wavelength of \({p}\) is

1 \({\lambda_{x}+\lambda_{y}}\)
2 \({\dfrac{\lambda_{x} \lambda_{y}}{\lambda_{x}+\lambda_{y}}}\)
3 \({\dfrac{\lambda_{x} \lambda_{y}}{\left|\lambda_{x}-\lambda_{y}\right|}}\)
4 \({\lambda_{x}-\lambda_{y}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357899 When a proton is accelerated with 1 volt potential difference, its kinetic energy is

1 1840 \(eV\)
2 1 \(eV\)
3 184 \(eV\)
4 18400 \(eV\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357900 A particle is dropped from a height ' \(H\) '. The de Broglie wavelength of the particle depends on height as

1 \(H\)
2 \({H^{ - 1/2}}\)
3 \({H^0}\)
4 \({H^{1/2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357896 Nuclear radii may be measured by scattering high energy electrons from nuclei. What is the de-Broglie wavelength for \(200\,M{\mkern 1mu} eV\) electrons?

1 \(8.28\,Fm\)
2 \(7.98\,Fm\)
3 \(6.45\,Fm\)
4 \(6.20\,Fm\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357897 An electron is accelerated from rest through a potential difference of \(\) volt. If the de Broglie wavelength of the electron is \(1.227 \times {10^{ - 2}}\;nm\), the potential difference is:

1 \({10^2}\;V\)
2 \({10^3}\;V\)
3 \({10^4}\;V\)
4 \(10\;V\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357898 A particle \({P}\) is formed due to a completely inelastic collision of particles \({x}\) and \({y}\), having de-Broglie wavelengths \({\lambda_{x}}\) and \({\lambda_{y}}\) respectively. If \({x}\) and \({y}\) were moving in opposite directions, then the de Broglie wavelength of \({p}\) is

1 \({\lambda_{x}+\lambda_{y}}\)
2 \({\dfrac{\lambda_{x} \lambda_{y}}{\lambda_{x}+\lambda_{y}}}\)
3 \({\dfrac{\lambda_{x} \lambda_{y}}{\left|\lambda_{x}-\lambda_{y}\right|}}\)
4 \({\lambda_{x}-\lambda_{y}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357899 When a proton is accelerated with 1 volt potential difference, its kinetic energy is

1 1840 \(eV\)
2 1 \(eV\)
3 184 \(eV\)
4 18400 \(eV\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357900 A particle is dropped from a height ' \(H\) '. The de Broglie wavelength of the particle depends on height as

1 \(H\)
2 \({H^{ - 1/2}}\)
3 \({H^0}\)
4 \({H^{1/2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357896 Nuclear radii may be measured by scattering high energy electrons from nuclei. What is the de-Broglie wavelength for \(200\,M{\mkern 1mu} eV\) electrons?

1 \(8.28\,Fm\)
2 \(7.98\,Fm\)
3 \(6.45\,Fm\)
4 \(6.20\,Fm\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357897 An electron is accelerated from rest through a potential difference of \(\) volt. If the de Broglie wavelength of the electron is \(1.227 \times {10^{ - 2}}\;nm\), the potential difference is:

1 \({10^2}\;V\)
2 \({10^3}\;V\)
3 \({10^4}\;V\)
4 \(10\;V\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357898 A particle \({P}\) is formed due to a completely inelastic collision of particles \({x}\) and \({y}\), having de-Broglie wavelengths \({\lambda_{x}}\) and \({\lambda_{y}}\) respectively. If \({x}\) and \({y}\) were moving in opposite directions, then the de Broglie wavelength of \({p}\) is

1 \({\lambda_{x}+\lambda_{y}}\)
2 \({\dfrac{\lambda_{x} \lambda_{y}}{\lambda_{x}+\lambda_{y}}}\)
3 \({\dfrac{\lambda_{x} \lambda_{y}}{\left|\lambda_{x}-\lambda_{y}\right|}}\)
4 \({\lambda_{x}-\lambda_{y}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357899 When a proton is accelerated with 1 volt potential difference, its kinetic energy is

1 1840 \(eV\)
2 1 \(eV\)
3 184 \(eV\)
4 18400 \(eV\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357900 A particle is dropped from a height ' \(H\) '. The de Broglie wavelength of the particle depends on height as

1 \(H\)
2 \({H^{ - 1/2}}\)
3 \({H^0}\)
4 \({H^{1/2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357896 Nuclear radii may be measured by scattering high energy electrons from nuclei. What is the de-Broglie wavelength for \(200\,M{\mkern 1mu} eV\) electrons?

1 \(8.28\,Fm\)
2 \(7.98\,Fm\)
3 \(6.45\,Fm\)
4 \(6.20\,Fm\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357897 An electron is accelerated from rest through a potential difference of \(\) volt. If the de Broglie wavelength of the electron is \(1.227 \times {10^{ - 2}}\;nm\), the potential difference is:

1 \({10^2}\;V\)
2 \({10^3}\;V\)
3 \({10^4}\;V\)
4 \(10\;V\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357898 A particle \({P}\) is formed due to a completely inelastic collision of particles \({x}\) and \({y}\), having de-Broglie wavelengths \({\lambda_{x}}\) and \({\lambda_{y}}\) respectively. If \({x}\) and \({y}\) were moving in opposite directions, then the de Broglie wavelength of \({p}\) is

1 \({\lambda_{x}+\lambda_{y}}\)
2 \({\dfrac{\lambda_{x} \lambda_{y}}{\lambda_{x}+\lambda_{y}}}\)
3 \({\dfrac{\lambda_{x} \lambda_{y}}{\left|\lambda_{x}-\lambda_{y}\right|}}\)
4 \({\lambda_{x}-\lambda_{y}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357899 When a proton is accelerated with 1 volt potential difference, its kinetic energy is

1 1840 \(eV\)
2 1 \(eV\)
3 184 \(eV\)
4 18400 \(eV\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357900 A particle is dropped from a height ' \(H\) '. The de Broglie wavelength of the particle depends on height as

1 \(H\)
2 \({H^{ - 1/2}}\)
3 \({H^0}\)
4 \({H^{1/2}}\)