The magnification \( m \) for a concave mirror is given by: \[ m = \frac{-v}{u} \] where \( v \) is the image distance and \( u \) is the object distance. We are given that \( m = -\frac{1}{9} \) for a real image, so: \[ \frac{-v}{u} = -\frac{1}{9} \] This implies: \[ v = \frac{u}{9} \] The mirror equation is: \[ \frac{1}{f} = \frac{1}{v} + \frac{1}{u} \] For a concave mirror, the focal length \( f \) is related to the radius of curvature \( R \) by: \[ f = \frac{R}{2} = \frac{36}{2} = 18 \, \text{cm} \] Substitute \( f = 18 \) cm into the mirror equation: \[ \frac{1}{18} = \frac{1}{v} + \frac{1}{u} \] Using the relation \( v = \frac{u}{9} \), substitute this into the equation: \[ \frac{1}{18} = \frac{9}{u} + \frac{1}{u} \] Simplifying: \[ \frac{1}{18} = \frac{10}{u} \] Solving for \( u \): \[ u = 180 \, \text{cm} \] Thus, the object should be placed 180 cm from the mirror.
\(XPQY\) is a vertical smooth long loop having a total resistance \(R\), where \(PX\) is parallel to \(QY\) and the separation between them is \(l\). A constant magnetic field \(B\) perpendicular to the plane of the loop exists in the entire space. A rod \(CD\) of length \(L\,(L>l)\) and mass \(m\) is made to slide down from rest under gravity as shown. The terminal speed acquired by the rod is _______ m/s. 
A biconvex lens is formed by using two plano-convex lenses as shown in the figure. The refractive index and radius of curvature of surfaces are also mentioned. When an object is placed on the left side of the lens at a distance of \(30\,\text{cm}\), the magnification of the image will be: 
In the system shown below, $x(t)=\sin(t)u(t)$. In steady-state, the response $y(t)$ will be 
The time constant of the network shown in the figure is 
The parallel RLC circuit shown in the figure is in resonance. In this circuit, 