Step 1: Magnetic flux (\( \Phi \)) linked with a coil depends on: \[ \Phi = B A \cos \theta \] where:
- \( B \) = Magnetic field strength
- \( A \) = Area of the coil
- \( \theta \) = Angle between the field and the normal to the coil \[ \boxed{\text{Flux depends on } B, A, \text{ and } \theta.} \]
(i) Cause
Solution: The changing magnetic field causes an induced electromotive force (EMF).
Step 1: According to Faraday's law, EMF is induced when the magnetic flux through a coil changes with time. \[ \mathcal{E} = -\frac{d\Phi}{dt} \] \[ \boxed{\text{Changing flux induces EMF.}} \]
(ii) Magnitude
Solution: The magnitude of induced EMF is proportional to the rate of change of flux.
Step 1: Using Faraday's law, the magnitude of the induced EMF is: \[ |\mathcal{E}| = \left| \frac{d\Phi}{dt} \right| \]
Step 2: Faster changes in flux result in higher EMF. \[ \boxed{\mathcal{E} \propto \frac{d\Phi}{dt}} \]
(iii) Direction
Solution: The direction of induced EMF is given by Lenz's Law.
Step 1: According to Lenz's Law, the induced EMF opposes the change in magnetic flux.
Step 2: The negative sign in Faraday's law signifies this opposition. \[ \mathcal{E} = -\frac{d\Phi}{dt} \] \[ \boxed{\text{Opposes the flux change.}} \]
Find the values of \( x, y, z \) if the matrix \( A \) satisfies the equation \( A^T A = I \), where
\[ A = \begin{bmatrix} 0 & 2y & z \\ x & y & -z \\ x & -y & z \end{bmatrix} \]
(b) Order of the differential equation: $ 5x^3 \frac{d^3y}{dx^3} - 3\left(\frac{dy}{dx}\right)^2 + \left(\frac{d^2y}{dx^2}\right)^4 + y = 0 $