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Question: The lens in an overhead projector forms an image of a point on an overhead transparency. If the scre...

The lens in an overhead projector forms an image of a point on an overhead transparency. If the screen is moved closer to the projector to keep the image on the screen in focus, the lens must be

(A) Moved Up
(B) Moved Towards Left
(C) Moved Down
(D) Moved Lens of Focal

Explanation

Solution

Hint
To solve this sum, we just need to know the lens formula which is given by 1v=1f+1u\dfrac{1}{v} = \dfrac{1}{f} + \dfrac{1}{u} and take into consideration the image which will be formed if the mirror is removed. The sign of the distance moved by the lens will give us the answer.
In this question, we will use the formula
1v=1f+1u\dfrac{1}{v} = \dfrac{1}{f} + \dfrac{1}{u}
where, vv is the image distance, uu is the object distance and ff is the local length of the lens.

Complete step by step answer

To solve this problem first, let us consider a situation where the mirror MM is removed. Then in that situation, the lines are extrapolated and the position of the image behind the mirror is seen asPP'.
So therefore here as we see in the image, we consider the initial distance between the object PP and the lens as u0{u_0}and the distance of the point PP' behind the mirror from the lens as the image distancev0{v_0}.
So considering the focal length of the lens to be ff, we can write from the lens formula,
1v0=1f+1u0\dfrac{1}{{{v_0}}} = \dfrac{1}{f} + \dfrac{1}{{{u_0}}}
Now according to the problem, the screen is moved closer to the projector. This means that the image PP' comes closer to the lens. From the image, let us consider that the screen is moved a distance xx such that the new image is formed at the position PP''.
So now to focus the image at PP'' the lens is further moved a distance of yy to the new position L2{{\text{L}}_{\text{2}}} . Now we need to find the sign of this variable yy which will give us the answer.
So again from this new condition, we can rewrite the lens formula again as,
1v0x=1f+1u0y\dfrac{1}{{{v_0} - x}} = \dfrac{1}{f} + \dfrac{1}{{{u_0} - y}}
We have already taken the variable xx to be positive. So we can say that,
1v0x>1v0\dfrac{1}{{{v_0} - x}} > \dfrac{1}{{{v_0}}}
1f+1u0y>1v0\Rightarrow \dfrac{1}{f} + \dfrac{1}{{{u_0} - y}} > \dfrac{1}{{{v_0}}}
Now we can substitute v0{v_0}from the initial lens formula as,
1f+1u0y>1f+1u0\dfrac{1}{f} + \dfrac{1}{{{u_0} - y}} > \dfrac{1}{f} + \dfrac{1}{{{u_0}}}
By canceling the 1f\dfrac{1}{f} on both the sides, we get
1u0y>1u0\dfrac{1}{{{u_0} - y}} > \dfrac{1}{{{u_0}}}
So this above equation is only possible when y is positive. So the Lens needs to be moved upwards.
So the correct option is A.

Note
We need to take special care of the sign conventions while doing problems in geometrical optics. In the case of the real image, if the object distance is taken as negative then the focal length and image distance are taken positively.