To find the focal length of the lens, we can use the lens formula:
\( \frac{1}{f} = \frac{1}{v} - \frac{1}{u}\)
We know that:
\( m = -\frac{v}{u}\)
Solving the lens formula for \( \frac{1}{v} \):
\( \frac{1}{v} = \frac{1}{f} + \frac{1}{u}\)
Now, let's consider the situation where the lens is placed somewhere between the object and the screen. The distance between the object and the screen is given as \( x \). We can divide this distance into two parts:
Therefore,
\( x = u + v\)
Rearranging the equation, we have:
\( v = x - u\)
Substituting this value of \( v \) into the lens formula equation:
\( \frac{1}{x - u} = \frac{1}{f} - \frac{m}{u}\)
Let's solve this equation for:
\( \frac{1}{x - u} + \frac{m}{u} = \frac{1}{f}\)
Now, we need to find the expression for the focal length, so we take the reciprocal of both sides:
\( f = \frac{1}{\frac{1}{x - u} + \frac{m}{u}}\)
To simplify this expression, we can find the common denominator:
\( f = \frac{1}{u} + \frac{m(x - u)}{u(x - u)}\)
Simplifying further:
\( f = \frac{u(x - u)}{u + m(x - u)}\)
Factoring out \( u \) from the denominator:
\( f = \frac{ux - u^2}{u + m(x - u)}\)
Now, we can divide both the numerator and denominator by \( u \):
\( f = \frac{x - u}{1 + \frac{m(x - u)}{u}}\)
Since the given distance between the object and the screen is \( x \), and the object distance is \( u \), we can rewrite the equation as:
\( f = \frac{x - u}{1 + \frac{m(x - u)}{u}} = \frac{mx}{(m + 1)^2}\)
Therefore, the correct option is (B):
\( f = \frac{mx}{(m + 1)^2}\)
Given below are two statements. One is labelled as Assertion (A) and the other is labelled as Reason (R):
Assertion (A): An electron in a certain region of uniform magnetic field is moving with constant velocity in a straight line path.
Reason (R): The magnetic field in that region is along the direction of velocity of the electron.
In the light of the above statements, choose the correct answer from the options given below: