Answer
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Hint:Center of curvature is twice as far as the focus of the concave mirror. Any light ray passing through the center of curvature will fall on the spherical surface in a perpendicular manner. Any light ray parallel to the principal axis will pass through the focus after reflection.
Complete step by step solution:
It is given that the object is kept between the center of curvature and focus.
We know that the radius of curvature is twice the focal length. Hence, we can place the object between the focus and center of curvature like we can see in the diagram.
First, draw a light ray passing through the center of curvature of the spherical surface. Any light passing through the center of curvature will fall on the spherical surface in a perpendicular manner. As a result, the light will trace back it’s the path. The BCB’ shows the path of the light ray in the diagram.
From the definition of the focus, we can say that any light, parallel to the principal axis, will go through the focus of the spherical surface after reflection. Hence, draw a light ray that is parallel to the principal axis. The light ray will pass through the focus of the spherical mirror after reflection.
The image of point B will be the point where these two light rays meet. In this case, the point is B’. So, A’B’ is the image of AB. As we can see, the image is real, inverted, and magnified.
Note:The same problem can be solved using the mirror formula. However, the process will take more calculation and mathematical manipulation. This solution uses the properties of spherical surfaces, and thereby, making the solution easy and universal.
Complete step by step solution:
It is given that the object is kept between the center of curvature and focus.
We know that the radius of curvature is twice the focal length. Hence, we can place the object between the focus and center of curvature like we can see in the diagram.
First, draw a light ray passing through the center of curvature of the spherical surface. Any light passing through the center of curvature will fall on the spherical surface in a perpendicular manner. As a result, the light will trace back it’s the path. The BCB’ shows the path of the light ray in the diagram.
From the definition of the focus, we can say that any light, parallel to the principal axis, will go through the focus of the spherical surface after reflection. Hence, draw a light ray that is parallel to the principal axis. The light ray will pass through the focus of the spherical mirror after reflection.
The image of point B will be the point where these two light rays meet. In this case, the point is B’. So, A’B’ is the image of AB. As we can see, the image is real, inverted, and magnified.
Note:The same problem can be solved using the mirror formula. However, the process will take more calculation and mathematical manipulation. This solution uses the properties of spherical surfaces, and thereby, making the solution easy and universal.
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