using the diagram above as a guide: Trace the outline ABC of the equilateral triangular glass prism provided. Remove the prism. Draw a line MN such that it ...
Trace the outline ABC of the equilateral triangular glass prism provided.
Remove the prism. Draw a line MN such that it makes an angle \(i = 5^\circ\) with the normal at N on side AB of the outline.
Fix two pins at \(P_{1}\) and \(P_{2}\) on MN. Replace the prism on its outline.
Looking through the face BC of the prism, fix one pin at \(P_{3}\) and another at \(P_{4}\) Such that they are in a straight line with the images of the pins at \(P_{1}\) and \(P_{2}\).
Remove the prism and the pins. Draw a line to join \(P_{4}\) and \(P_{3}\). Produce line \(P_{4}P_{3}\) to meet the line BC of the outline at CQ and line MN produced at P.
Draw a normal to BC at Q. Measure and record the angles \(\theta\) and e. Evaluate \(\phi = i + e\).
Repeat the procedure, using a different outline in each case, for four other values of \(i = 100\), \(159\), \(20\), and \(25\) respectively. Evaluate \(\phi = i + e\) in each case. Tabulate your readings.
Plot a graph of \(\theta\) on the vertical axis against \(\phi\) on the horizontal axis starting both axes from the origin \((0,0)\).
Determine the slope of the graph and the intercept on the vertical axis.
State two precautions taken to ensure accurate results.
(b)i. Explain what is meant by the statement: the refractive index of glass is 1.5.
ii. Calculate the critical angle of a medium of refractive index 1.65 when light passes from the medium to air.
Principle. A ray of light strikes face AB of the equilateral glass prism at an angle of incidence \(i\) to the normal, is refracted through the glass and emerges from face BC at an angle of emergence \(e\). For each setting the angle \(\theta\) at Q and the emergence angle \(e\) are measured, and \(\phi = i + e\) is evaluated. A graph of \(\theta\) against \(\phi\) is a straight line whose slope and vertical intercept are then read off.
Ray-tracing set-up.
Ray path through the equilateral prism: incidence at face AB and emergence at face BC, with pins P1-P4 and normals.
Trace the outline ABC, draw MN at the required angle \(i\) to the normal at N on AB and fix pins P\(_1\), P\(_2\). Replace the prism, and looking through face BC fix pins P\(_3\), P\(_4\) in line with the images of P\(_1\) and P\(_2\). Join and produce P\(_4\)P\(_3\) to meet BC at Q, draw the normal at Q, then measure \(\theta\) and \(e\).
The line cuts the vertical axis at \(\phi = 0\), giving an intercept \(\theta_{\text{intercept}} = 120^\circ\).
Two precautions.
The object pins and image pins were fixed erect and viewed with one eye so that they and the images lay in one straight line, avoiding parallax error.
A sharp pencil was used for tracing the outline and marking pin positions, and the protractor was read squarely to obtain accurate angles.
(b)(i) The statement that the refractive index of glass is 1.5 means that the speed (or wavelength) of light in air is 1.5 times its speed (or wavelength) in the glass:
\[ n = \frac{\text{speed of light in air}}{\text{speed of light in glass}} = \frac{3}{2} = 1.5 \]
Equivalently, for a ray passing from air into the glass, \(\dfrac{\sin i}{\sin r} = 1.5\).
(b)(ii) Critical angle. At the critical angle \(C\) the ray inside the glass just grazes the surface, so
Principle. A ray of light strikes face AB of the equilateral glass prism at an angle of incidence \(i\) to the normal, is refracted through the glass and emerges from face BC at an angle of emergence \(e\). For each setting the angle \(\theta\) at Q and the emergence angle \(e\) are measured, and \(\phi = i + e\) is evaluated. A graph of \(\theta\) against \(\phi\) is a straight line whose slope and vertical intercept are then read off.
Ray-tracing set-up.
Ray path through the equilateral prism: incidence at face AB and emergence at face BC, with pins P1-P4 and normals.
Trace the outline ABC, draw MN at the required angle \(i\) to the normal at N on AB and fix pins P\(_1\), P\(_2\). Replace the prism, and looking through face BC fix pins P\(_3\), P\(_4\) in line with the images of P\(_1\) and P\(_2\). Join and produce P\(_4\)P\(_3\) to meet BC at Q, draw the normal at Q, then measure \(\theta\) and \(e\).
The line cuts the vertical axis at \(\phi = 0\), giving an intercept \(\theta_{\text{intercept}} = 120^\circ\).
Two precautions.
The object pins and image pins were fixed erect and viewed with one eye so that they and the images lay in one straight line, avoiding parallax error.
A sharp pencil was used for tracing the outline and marking pin positions, and the protractor was read squarely to obtain accurate angles.
(b)(i) The statement that the refractive index of glass is 1.5 means that the speed (or wavelength) of light in air is 1.5 times its speed (or wavelength) in the glass:
\[ n = \frac{\text{speed of light in air}}{\text{speed of light in glass}} = \frac{3}{2} = 1.5 \]
Equivalently, for a ray passing from air into the glass, \(\dfrac{\sin i}{\sin r} = 1.5\).
(b)(ii) Critical angle. At the critical angle \(C\) the ray inside the glass just grazes the surface, so