362801 A cyclotron is used to accelerate

362802 Frequency of cyclotron does not depend upon

362803 A cyclotron has an oscillator frequency 12\(MHz\) and a dee of radius 50\(cm\). The magnetic induction needed to accelerate deuterons of mass \(3.3 \times {10^{ - 27}}\;kg\) and charge \(1.6 \times {10^{ - 19}}\;kg\) is

362805 In a mass spectrometer used for measuring the masses of ions, the ions are initially accelerated by an electric potential \(V\) and then made to describe semicircular paths of radius \(R\) using a magnetic field \(B\). If \(V\) and \(B\) are kept constant, then the ratio\(\left. {\left( {\frac{{{\rm{charge}}\,\,{\rm{on}}\,\,{\rm{the}}\,\,{\rm{ion}}}}{{{\rm{mass}}\,\,{\rm{of}}\,\,{\rm{the}}\,\,{\rm{ion}}}}} \right.} \right)\)will be proportional to

362801 A cyclotron is used to accelerate

362802 Frequency of cyclotron does not depend upon

362803 A cyclotron has an oscillator frequency 12\(MHz\) and a dee of radius 50\(cm\). The magnetic induction needed to accelerate deuterons of mass \(3.3 \times {10^{ - 27}}\;kg\) and charge \(1.6 \times {10^{ - 19}}\;kg\) is

362805 In a mass spectrometer used for measuring the masses of ions, the ions are initially accelerated by an electric potential \(V\) and then made to describe semicircular paths of radius \(R\) using a magnetic field \(B\). If \(V\) and \(B\) are kept constant, then the ratio\(\left. {\left( {\frac{{{\rm{charge}}\,\,{\rm{on}}\,\,{\rm{the}}\,\,{\rm{ion}}}}{{{\rm{mass}}\,\,{\rm{of}}\,\,{\rm{the}}\,\,{\rm{ion}}}}} \right.} \right)\)will be proportional to

362801 A cyclotron is used to accelerate

362802 Frequency of cyclotron does not depend upon

362803 A cyclotron has an oscillator frequency 12\(MHz\) and a dee of radius 50\(cm\). The magnetic induction needed to accelerate deuterons of mass \(3.3 \times {10^{ - 27}}\;kg\) and charge \(1.6 \times {10^{ - 19}}\;kg\) is

362805 In a mass spectrometer used for measuring the masses of ions, the ions are initially accelerated by an electric potential \(V\) and then made to describe semicircular paths of radius \(R\) using a magnetic field \(B\). If \(V\) and \(B\) are kept constant, then the ratio\(\left. {\left( {\frac{{{\rm{charge}}\,\,{\rm{on}}\,\,{\rm{the}}\,\,{\rm{ion}}}}{{{\rm{mass}}\,\,{\rm{of}}\,\,{\rm{the}}\,\,{\rm{ion}}}}} \right.} \right)\)will be proportional to

362801 A cyclotron is used to accelerate

362802 Frequency of cyclotron does not depend upon

362803 A cyclotron has an oscillator frequency 12\(MHz\) and a dee of radius 50\(cm\). The magnetic induction needed to accelerate deuterons of mass \(3.3 \times {10^{ - 27}}\;kg\) and charge \(1.6 \times {10^{ - 19}}\;kg\) is

362805 In a mass spectrometer used for measuring the masses of ions, the ions are initially accelerated by an electric potential \(V\) and then made to describe semicircular paths of radius \(R\) using a magnetic field \(B\). If \(V\) and \(B\) are kept constant, then the ratio\(\left. {\left( {\frac{{{\rm{charge}}\,\,{\rm{on}}\,\,{\rm{the}}\,\,{\rm{ion}}}}{{{\rm{mass}}\,\,{\rm{of}}\,\,{\rm{the}}\,\,{\rm{ion}}}}} \right.} \right)\)will be proportional to