358146 Assertion :
If the medium between two charges is replaced by another medium of dielectric constant then the electric force between them decreases.
Reason :
Electric dipole moment varies inversely as the dielectric constant.

358147 The formation of a dipole is due to two equal and dissimilar point charges placed at a

358148 A region surrounding a stationary electric dipoles has

358149 An electric dipole is placed along the \(x\)-axis at the origin \(O\). A point \(P\) is at a distance of 10 \(cm\) from this origin such that \(OP\) makes an angle \(\frac{\pi }{6}\) with \(x\)-axis. If the electric field at \(P\) makes an angle \(\beta \) with the \(x\)-axis, the value of \(\beta \) would be

358150 The direction of electric field intensity \((\overrightarrow E )\) at a point on the equtorial line of an electric dipole of dipole moment \((\overrightarrow p )\) is

358146 Assertion :
If the medium between two charges is replaced by another medium of dielectric constant then the electric force between them decreases.
Reason :
Electric dipole moment varies inversely as the dielectric constant.

358147 The formation of a dipole is due to two equal and dissimilar point charges placed at a

358148 A region surrounding a stationary electric dipoles has

358149 An electric dipole is placed along the \(x\)-axis at the origin \(O\). A point \(P\) is at a distance of 10 \(cm\) from this origin such that \(OP\) makes an angle \(\frac{\pi }{6}\) with \(x\)-axis. If the electric field at \(P\) makes an angle \(\beta \) with the \(x\)-axis, the value of \(\beta \) would be

358150 The direction of electric field intensity \((\overrightarrow E )\) at a point on the equtorial line of an electric dipole of dipole moment \((\overrightarrow p )\) is

358146 Assertion :
If the medium between two charges is replaced by another medium of dielectric constant then the electric force between them decreases.
Reason :
Electric dipole moment varies inversely as the dielectric constant.

358147 The formation of a dipole is due to two equal and dissimilar point charges placed at a

358148 A region surrounding a stationary electric dipoles has

358149 An electric dipole is placed along the \(x\)-axis at the origin \(O\). A point \(P\) is at a distance of 10 \(cm\) from this origin such that \(OP\) makes an angle \(\frac{\pi }{6}\) with \(x\)-axis. If the electric field at \(P\) makes an angle \(\beta \) with the \(x\)-axis, the value of \(\beta \) would be

358150 The direction of electric field intensity \((\overrightarrow E )\) at a point on the equtorial line of an electric dipole of dipole moment \((\overrightarrow p )\) is

358146 Assertion :
If the medium between two charges is replaced by another medium of dielectric constant then the electric force between them decreases.
Reason :
Electric dipole moment varies inversely as the dielectric constant.

358147 The formation of a dipole is due to two equal and dissimilar point charges placed at a

358148 A region surrounding a stationary electric dipoles has

358149 An electric dipole is placed along the \(x\)-axis at the origin \(O\). A point \(P\) is at a distance of 10 \(cm\) from this origin such that \(OP\) makes an angle \(\frac{\pi }{6}\) with \(x\)-axis. If the electric field at \(P\) makes an angle \(\beta \) with the \(x\)-axis, the value of \(\beta \) would be

358150 The direction of electric field intensity \((\overrightarrow E )\) at a point on the equtorial line of an electric dipole of dipole moment \((\overrightarrow p )\) is

358146 Assertion :
If the medium between two charges is replaced by another medium of dielectric constant then the electric force between them decreases.
Reason :
Electric dipole moment varies inversely as the dielectric constant.

358147 The formation of a dipole is due to two equal and dissimilar point charges placed at a

358148 A region surrounding a stationary electric dipoles has

358149 An electric dipole is placed along the \(x\)-axis at the origin \(O\). A point \(P\) is at a distance of 10 \(cm\) from this origin such that \(OP\) makes an angle \(\frac{\pi }{6}\) with \(x\)-axis. If the electric field at \(P\) makes an angle \(\beta \) with the \(x\)-axis, the value of \(\beta \) would be

358150 The direction of electric field intensity \((\overrightarrow E )\) at a point on the equtorial line of an electric dipole of dipole moment \((\overrightarrow p )\) is