Given Information:
Speed of object, \( v_o = 1\,ms^{-1} \)
Speed of image, \( v_i = 1\,ms^{-1} \)
Focal length of convex lens, \( f = 10\,cm \)
Step-by-Step Explanation:
Step 1: Relation between object speed and image speed
Using lens formula: \[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \] where:
\( u \) = object distance (negative for real objects),
\( v \) = image distance (positive for real images).
Step 2: Differentiate lens formula with respect to time to find relation between velocities
Differentiating both sides: \[ 0 = -\frac{1}{v^2}\frac{dv}{dt} + \frac{1}{u^2}\frac{du}{dt} \]
Thus, \[ \frac{dv}{dt} = \frac{v^2}{u^2}\frac{du}{dt} \]
Given, \( |\frac{dv}{dt}| = |\frac{du}{dt}| \), thus: \[ \frac{v^2}{u^2} = 1 \quad\Rightarrow\quad v^2 = u^2 \]
Thus, \( v = u \) (since distances are positive for simplicity).
Step 3: Use \( v = u \) in lens formula to find object distance
From lens formula: \[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u}, \quad\text{and since}\quad v = u: \]
\[ \frac{1}{f} = \frac{1}{u} - \frac{1}{u} = 0 \]
But this leads to a contradiction if we directly substitute \( v = u \). Hence, let's carefully reconsider signs:
For a real object, \( u \) is negative and \( v \) is positive. Therefore, the correct condition considering signs becomes: \[ v = -u \]
Substitute \( v = -u \) into lens formula carefully: \[ \frac{1}{f} = \frac{1}{-u} - \frac{1}{u} = -\frac{2}{u} \]
Thus: \[ -\frac{2}{u} = \frac{1}{f} \quad\Rightarrow\quad u = -2f \]
Since \( f = 10\,cm \), object distance is: \[ u = -2 \times 10\,cm = -20\,cm \]
Thus, the object must be at \(20\,cm\) from the lens.
We use the lens formula: \[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \] where: - \( f \) is the focal length of the lens, - \( v \) is the image distance, - \( u \) is the object distance. The relationship between the speed of the object \( v_o \) and the speed of the image \( v_i \) can be written as: \[ \frac{v_i}{v_o} = \left|\frac{v}{u}\right| \] Given that the speed of the object is \( v_o = 1 \, \text{m/s} \) and the speed of the image is also \( v_i = 1 \, \text{m/s} \), we can substitute into the equation: \[ 1 = \left|\frac{v}{u}\right| \] The focal length is \( f = 10 \, \text{cm} = 0.1 \, \text{m} \), so using the lens formula: \[ \frac{1}{0.1} = \frac{1}{v} - \frac{1}{u} \] Solving this equation gives: \[ \frac{1}{v} = \frac{1}{0.1} + \frac{1}{u} \] For the speed of the image to be equal to the speed of the object, the object distance must be at \( u = -20 \, \text{cm} \).
Thus, the object is 20 cm away from the lens.
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is