(i)
When a ray of light passes through a rectangular glass slab, it refracts at two parallel faces — AB (air to glass) and CD (glass to air). The bending at these two faces is equal and opposite because the faces are parallel to each other. Hence, the emergent ray comes out parallel to the incident ray, though it is laterally displaced.
Ray Diagram:
```
E N
\ |
\i |
----O-------+---- AB (air-glass)
|r |
OO'(refracted ray)
----O'------+---- CD (glass-air)
| |
\ M'
H (emergent, parallel to EO)
```
When light falls normally on a face: The angle of incidence = 0°, so the ray passes straight through without any bending (no refraction). It continues in the same direction.
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(ii)
Given: $u = -30$ cm, $f = -20$ cm (concave lens)
Using lens formula:
$$\frac{1}{v} - \frac{1}{u} = \frac{1}{f}$$
$$\frac{1}{v} = \frac{1}{f} + \frac{1}{u} = \frac{1}{-20} + \frac{1}{-30}$$
$$\frac{1}{v} = \frac{-3 - 2}{60} = \frac{-5}{60} = \frac{-1}{12}$$
$$v = -12 \text{ cm}$$
The image is formed 12 cm in front of the lens (on the same side as the object). It is virtual and erect.
Source: Chapter 9, Section 9.3.1 (Refraction through a Rectangular Glass Slab) and Sign Convention for Spherical Lenses
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