266293 The number of turns of primary and secondary coils of a transformer are 5 and 10 respectively and the mutual inductance of the transformer is 25 henry. Now the number of turns in the primary and secondary of the transformer are made 10 and 5 respectively. The mutual inductance of the transformer in henry will be:

266294 Statement I: The Q value of a nuclear process given by \(\mathrm{Q}=\) final kinetic energy - initial kinetic energy Statement II: The Q value of nuclear process is \(Q=\) (sum of final masses - sum of initial masses) \(\times \mathrm{C}^2\)

266295 When unpolarised light beam is incident from air into glass ( \(\mathrm{n}=\mathbf{1 . 5}\) ) at the polarising angle:

266296 Statement I: The binding energy per nucleon, \(\mathrm{E}_{\mathrm{in}}\), is practically constant, i.e. practically independent of the atomic number for nuclei of middle mass number ( \(30<\mathrm{A}<170\) ). The curve has a maximum of about 8.75 MeV for \(\mathrm{A}=56\) and has a value of 7.6 MeV for \(\mathrm{A}=238\). Statement II : \(\mathrm{E}_{\mathrm{tn}}\) is lower for both light nuclei ( \(A<30\) ) and heavy nuclei ( \(A>170\) ) in comparison to \(\mathrm{E}_{\mathrm{m}}\) of nuclei of intermediate atomic number.

266293 The number of turns of primary and secondary coils of a transformer are 5 and 10 respectively and the mutual inductance of the transformer is 25 henry. Now the number of turns in the primary and secondary of the transformer are made 10 and 5 respectively. The mutual inductance of the transformer in henry will be:

266294 Statement I: The Q value of a nuclear process given by \(\mathrm{Q}=\) final kinetic energy - initial kinetic energy Statement II: The Q value of nuclear process is \(Q=\) (sum of final masses - sum of initial masses) \(\times \mathrm{C}^2\)

266295 When unpolarised light beam is incident from air into glass ( \(\mathrm{n}=\mathbf{1 . 5}\) ) at the polarising angle:

266296 Statement I: The binding energy per nucleon, \(\mathrm{E}_{\mathrm{in}}\), is practically constant, i.e. practically independent of the atomic number for nuclei of middle mass number ( \(30<\mathrm{A}<170\) ). The curve has a maximum of about 8.75 MeV for \(\mathrm{A}=56\) and has a value of 7.6 MeV for \(\mathrm{A}=238\). Statement II : \(\mathrm{E}_{\mathrm{tn}}\) is lower for both light nuclei ( \(A<30\) ) and heavy nuclei ( \(A>170\) ) in comparison to \(\mathrm{E}_{\mathrm{m}}\) of nuclei of intermediate atomic number.

266293 The number of turns of primary and secondary coils of a transformer are 5 and 10 respectively and the mutual inductance of the transformer is 25 henry. Now the number of turns in the primary and secondary of the transformer are made 10 and 5 respectively. The mutual inductance of the transformer in henry will be:

266294 Statement I: The Q value of a nuclear process given by \(\mathrm{Q}=\) final kinetic energy - initial kinetic energy Statement II: The Q value of nuclear process is \(Q=\) (sum of final masses - sum of initial masses) \(\times \mathrm{C}^2\)

266295 When unpolarised light beam is incident from air into glass ( \(\mathrm{n}=\mathbf{1 . 5}\) ) at the polarising angle:

266296 Statement I: The binding energy per nucleon, \(\mathrm{E}_{\mathrm{in}}\), is practically constant, i.e. practically independent of the atomic number for nuclei of middle mass number ( \(30<\mathrm{A}<170\) ). The curve has a maximum of about 8.75 MeV for \(\mathrm{A}=56\) and has a value of 7.6 MeV for \(\mathrm{A}=238\). Statement II : \(\mathrm{E}_{\mathrm{tn}}\) is lower for both light nuclei ( \(A<30\) ) and heavy nuclei ( \(A>170\) ) in comparison to \(\mathrm{E}_{\mathrm{m}}\) of nuclei of intermediate atomic number.

266293 The number of turns of primary and secondary coils of a transformer are 5 and 10 respectively and the mutual inductance of the transformer is 25 henry. Now the number of turns in the primary and secondary of the transformer are made 10 and 5 respectively. The mutual inductance of the transformer in henry will be:

266294 Statement I: The Q value of a nuclear process given by \(\mathrm{Q}=\) final kinetic energy - initial kinetic energy Statement II: The Q value of nuclear process is \(Q=\) (sum of final masses - sum of initial masses) \(\times \mathrm{C}^2\)

266295 When unpolarised light beam is incident from air into glass ( \(\mathrm{n}=\mathbf{1 . 5}\) ) at the polarising angle:

266296 Statement I: The binding energy per nucleon, \(\mathrm{E}_{\mathrm{in}}\), is practically constant, i.e. practically independent of the atomic number for nuclei of middle mass number ( \(30<\mathrm{A}<170\) ). The curve has a maximum of about 8.75 MeV for \(\mathrm{A}=56\) and has a value of 7.6 MeV for \(\mathrm{A}=238\). Statement II : \(\mathrm{E}_{\mathrm{tn}}\) is lower for both light nuclei ( \(A<30\) ) and heavy nuclei ( \(A>170\) ) in comparison to \(\mathrm{E}_{\mathrm{m}}\) of nuclei of intermediate atomic number.