Ana loda....
|
Latsa & Riƙe don Ja Shi Gabaɗaya |
|||
|
Danna nan don rufewa |
|||
Tambaya 1 Rahoto
You are provided with a potentiometer XY, a voltmeter, V, a standard resistor R, an accumulator, E a plug key, K, a jockey, and connecting wires.
(b)i. State four factors on which the resistance of a wire depends.
ii. A resistance Wire of length 100cm is connected in a circuit. If the resistance per unit length of the wire is 0.02 \(\Omega\)cm\(^{-1}\), how much heat would be produced in the wire if a voltmeter connected across its ends indicates 1.5V while the current runs for 1 minute?
Circuit: The accumulator \(E\), key \(K\) and standard resistor \(R\) are joined in series with the potentiometer wire \(XY\). The voltmeter \(V\) is connected between \(X\) and the jockey, so it reads the potential difference across the length \(l = XN\).
With the key closed, the jockey is pressed at \(N\) so that \(l = XN = 15.0\,\text{cm}\) and the voltmeter reading \(V\) is recorded. The procedure is repeated for \(l = 25.0, 35.0, 45.0, 55.0\) and \(65.0\,\text{cm}\). For each length \(l^{-1}\) and \(V^{-1}\) are evaluated.
| S/N | \(l\,/\,\text{cm}\) | \(V\,/\,\text{volt}\) | \(l^{-1}\,/\,\text{cm}^{-1}\) | \(V^{-1}\,/\,\text{volt}^{-1}\) |
|---|---|---|---|---|
| 1 | 15.0 | 0.60 | 0.0667 | 1.667 |
| 2 | 25.0 | 0.80 | 0.0400 | 1.250 |
| 3 | 35.0 | 1.10 | 0.0286 | 0.909 |
| 4 | 45.0 | 1.30 | 0.0222 | 0.769 |
| 5 | 55.0 | 1.60 | 0.0182 | 0.625 |
| 6 | 65.0 | 1.80 | 0.0154 | 0.556 |
Worked evaluations (row 1): \(l^{-1}=\dfrac{1}{15.0}=0.0667\,\text{cm}^{-1}\), \(V^{-1}=\dfrac{1}{0.60}=1.667\,\text{volt}^{-1}\); (row 6): \(l^{-1}=\dfrac{1}{65.0}=0.0154\,\text{cm}^{-1}\), \(V^{-1}=\dfrac{1}{1.80}=0.556\,\text{volt}^{-1}\).
Using two points on the line of best fit, \((l^{-1}=0.0154,\ V^{-1}=0.603)\) and \((l^{-1}=0.0667,\ V^{-1}=1.724)\):
\[ s=\frac{\Delta V^{-1}}{\Delta l^{-1}}=\frac{1.724-0.603}{0.0667-0.0154}=\frac{1.121}{0.0513}=21.85\ \text{cm}\,\text{volt}^{-1}. \]Resistance of the wire:
\[ R = (\text{resistance per unit length})\times(\text{length}) = 0.02\times100 = 2\,\Omega. \]Given \(V=1.5\,\text{V}\) and \(t=1\,\text{minute}=60\,\text{s}\), the heat produced is
\[ H=\frac{V^{2}t}{R}=\frac{(1.5)^{2}\times60}{2}=\frac{2.25\times60}{2}=\frac{135}{2}=67.5\,\text{J}. \]Check (using current): \(I=\dfrac{V}{R}=\dfrac{1.5}{2}=0.75\,\text{A}\), so \(H=I^{2}Rt=(0.75)^{2}\times2\times60=0.5625\times120=67.5\,\text{J}.\)
Bayanin Amsa
Circuit: The accumulator \(E\), key \(K\) and standard resistor \(R\) are joined in series with the potentiometer wire \(XY\). The voltmeter \(V\) is connected between \(X\) and the jockey, so it reads the potential difference across the length \(l = XN\).
With the key closed, the jockey is pressed at \(N\) so that \(l = XN = 15.0\,\text{cm}\) and the voltmeter reading \(V\) is recorded. The procedure is repeated for \(l = 25.0, 35.0, 45.0, 55.0\) and \(65.0\,\text{cm}\). For each length \(l^{-1}\) and \(V^{-1}\) are evaluated.
| S/N | \(l\,/\,\text{cm}\) | \(V\,/\,\text{volt}\) | \(l^{-1}\,/\,\text{cm}^{-1}\) | \(V^{-1}\,/\,\text{volt}^{-1}\) |
|---|---|---|---|---|
| 1 | 15.0 | 0.60 | 0.0667 | 1.667 |
| 2 | 25.0 | 0.80 | 0.0400 | 1.250 |
| 3 | 35.0 | 1.10 | 0.0286 | 0.909 |
| 4 | 45.0 | 1.30 | 0.0222 | 0.769 |
| 5 | 55.0 | 1.60 | 0.0182 | 0.625 |
| 6 | 65.0 | 1.80 | 0.0154 | 0.556 |
Worked evaluations (row 1): \(l^{-1}=\dfrac{1}{15.0}=0.0667\,\text{cm}^{-1}\), \(V^{-1}=\dfrac{1}{0.60}=1.667\,\text{volt}^{-1}\); (row 6): \(l^{-1}=\dfrac{1}{65.0}=0.0154\,\text{cm}^{-1}\), \(V^{-1}=\dfrac{1}{1.80}=0.556\,\text{volt}^{-1}\).
Using two points on the line of best fit, \((l^{-1}=0.0154,\ V^{-1}=0.603)\) and \((l^{-1}=0.0667,\ V^{-1}=1.724)\):
\[ s=\frac{\Delta V^{-1}}{\Delta l^{-1}}=\frac{1.724-0.603}{0.0667-0.0154}=\frac{1.121}{0.0513}=21.85\ \text{cm}\,\text{volt}^{-1}. \]Resistance of the wire:
\[ R = (\text{resistance per unit length})\times(\text{length}) = 0.02\times100 = 2\,\Omega. \]Given \(V=1.5\,\text{V}\) and \(t=1\,\text{minute}=60\,\text{s}\), the heat produced is
\[ H=\frac{V^{2}t}{R}=\frac{(1.5)^{2}\times60}{2}=\frac{2.25\times60}{2}=\frac{135}{2}=67.5\,\text{J}. \]Check (using current): \(I=\dfrac{V}{R}=\dfrac{1.5}{2}=0.75\,\text{A}\), so \(H=I^{2}Rt=(0.75)^{2}\times2\times60=0.5625\times120=67.5\,\text{J}.\)
Tambaya 2 Rahoto
You have been provided with a retort stand, clamp and boss, a set of masses, a spiral spring, stopwatch, split cork, and other necessary apparatus. Using the diagram above as a guide, carry out the following instructions;
(b)i. Define Young modulus and force constant.
ii. A force of magnitude 500N is applied to the free end of a spiral spring of force constant 1.0 x 10\(^{4}\) Nm\(^{-1}\). Calculate the energy stored in the stretched spring.
For each load, the time for 20 complete oscillations was measured twice. The mean time is \(t\), hence
\[T=\frac{t}{20},\qquad T^2=\left(\frac{t}{20}\right)^2.\]
| Mass, \(m\) (g) | \(t_1\) (s) | \(t_2\) (s) | Mean \(t\) for 20 oscillations (s) | Period, \(T=t/20\) (s) | \(T^2\) (s2) | \(T^2\times10^3\) (s2) |
|---|---|---|---|---|---|---|
| 50.0 | 5.80 | 5.80 | 5.80 | 0.290 | 0.084 | 84 |
| 70.0 | 6.70 | 6.90 | 6.80 | 0.340 | 0.116 | 116 |
| 90.0 | 7.80 | 8.00 | 7.90 | 0.395 | 0.156 | 156 |
| 110.0 | 8.50 | 8.70 | 8.60 | 0.430 | 0.185 | 185 |
| 130.0 | 9.20 | 9.20 | 9.20 | 0.460 | 0.212 | 212 |
The graph is plotted with \(T^2\times10^3\) on the vertical axis and mass on the horizontal axis.
Using two widely separated points on the straight line, \((m,T^2\times10^3)=(6,10)\) and \((140,234)\),
\[s=\frac{(234-10)\times10^{-3}}{140-6}=1.672\times10^{-3}\ \text{s}^2\text{g}^{-1}=1.672\ \text{s}^2\text{kg}^{-1}.\]
The vertical intercept, \(l\), is approximately \(0\ \text{s}^2\).
Since \(T^2=\dfrac{4\pi^2}{k}m\),
\[k=\frac{4\pi^2}{s}=\frac{4\left(\frac{22}{7}\right)^2}{1.672}=23.6\ \text{N m}^{-1}.\]
Young modulus is the ratio of tensile stress to tensile strain, provided the elastic limit is not exceeded:
\[E=\frac{F/A}{e/L}=\frac{FL}{Ae}.\]
Force constant is the force required to produce unit extension of a spring:
\[k=\frac{F}{e}.\]
\[e=\frac{F}{k}=\frac{500}{1.0\times10^4}=0.050\ \text{m}.\]
\[W=\frac{1}{2}Fe=\frac{1}{2}\times500\times0.050=12.5\ \text{J}.\]
Bayanin Amsa
For each load, the time for 20 complete oscillations was measured twice. The mean time is \(t\), hence
\[T=\frac{t}{20},\qquad T^2=\left(\frac{t}{20}\right)^2.\]
| Mass, \(m\) (g) | \(t_1\) (s) | \(t_2\) (s) | Mean \(t\) for 20 oscillations (s) | Period, \(T=t/20\) (s) | \(T^2\) (s2) | \(T^2\times10^3\) (s2) |
|---|---|---|---|---|---|---|
| 50.0 | 5.80 | 5.80 | 5.80 | 0.290 | 0.084 | 84 |
| 70.0 | 6.70 | 6.90 | 6.80 | 0.340 | 0.116 | 116 |
| 90.0 | 7.80 | 8.00 | 7.90 | 0.395 | 0.156 | 156 |
| 110.0 | 8.50 | 8.70 | 8.60 | 0.430 | 0.185 | 185 |
| 130.0 | 9.20 | 9.20 | 9.20 | 0.460 | 0.212 | 212 |
The graph is plotted with \(T^2\times10^3\) on the vertical axis and mass on the horizontal axis.
Using two widely separated points on the straight line, \((m,T^2\times10^3)=(6,10)\) and \((140,234)\),
\[s=\frac{(234-10)\times10^{-3}}{140-6}=1.672\times10^{-3}\ \text{s}^2\text{g}^{-1}=1.672\ \text{s}^2\text{kg}^{-1}.\]
The vertical intercept, \(l\), is approximately \(0\ \text{s}^2\).
Since \(T^2=\dfrac{4\pi^2}{k}m\),
\[k=\frac{4\pi^2}{s}=\frac{4\left(\frac{22}{7}\right)^2}{1.672}=23.6\ \text{N m}^{-1}.\]
Young modulus is the ratio of tensile stress to tensile strain, provided the elastic limit is not exceeded:
\[E=\frac{F/A}{e/L}=\frac{FL}{Ae}.\]
Force constant is the force required to produce unit extension of a spring:
\[k=\frac{F}{e}.\]
\[e=\frac{F}{k}=\frac{500}{1.0\times10^4}=0.050\ \text{m}.\]
\[W=\frac{1}{2}Fe=\frac{1}{2}\times500\times0.050=12.5\ \text{J}.\]
Tambaya 3 Rahoto
using the diagram above as a guide:
(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.
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 \(e\).
Table of readings.
| S/N | \(i\) (°) | \(e\) (°) | \(\theta\) (°) | \(\phi=i+e\) (°) |
|---|---|---|---|---|
| 1 | 5.0 | 5.0 | 130.0 | 10.0 |
| 2 | 10.0 | 10.0 | 140.0 | 20.0 |
| 3 | 15.0 | 15.0 | 150.0 | 30.0 |
| 4 | 20.0 | 20.0 | 160.0 | 40.0 |
| 5 | 25.0 | 25.0 | 170.0 | 50.0 |
Graph of \(\theta\) against \(\phi\).
Slope and intercept. Taking two widely separated points on the line of best fit, \((\phi_1,\theta_1)=(0,120)\) and \((\phi_2,\theta_2)=(50,170)\):
\[ \text{slope} = \frac{\Delta\theta}{\Delta\phi} = \frac{170-120}{50-0} = \frac{50}{50} = 1.0 \]The line cuts the vertical axis at \(\phi = 0\), giving an intercept \(\theta_{\text{intercept}} = 120^\circ\).
Two precautions.
(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
\[ {}_{a}n_{g} = \frac{1}{\sin C} \;\Rightarrow\; \sin C = \frac{1}{n} = \frac{1}{1.65} = 0.6061 \]\[ C = \sin^{-1}(0.6061) = 37.3^\circ \]Bayanin Amsa
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.
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 \(e\).
Table of readings.
| S/N | \(i\) (°) | \(e\) (°) | \(\theta\) (°) | \(\phi=i+e\) (°) |
|---|---|---|---|---|
| 1 | 5.0 | 5.0 | 130.0 | 10.0 |
| 2 | 10.0 | 10.0 | 140.0 | 20.0 |
| 3 | 15.0 | 15.0 | 150.0 | 30.0 |
| 4 | 20.0 | 20.0 | 160.0 | 40.0 |
| 5 | 25.0 | 25.0 | 170.0 | 50.0 |
Graph of \(\theta\) against \(\phi\).
Slope and intercept. Taking two widely separated points on the line of best fit, \((\phi_1,\theta_1)=(0,120)\) and \((\phi_2,\theta_2)=(50,170)\):
\[ \text{slope} = \frac{\Delta\theta}{\Delta\phi} = \frac{170-120}{50-0} = \frac{50}{50} = 1.0 \]The line cuts the vertical axis at \(\phi = 0\), giving an intercept \(\theta_{\text{intercept}} = 120^\circ\).
Two precautions.
(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
\[ {}_{a}n_{g} = \frac{1}{\sin C} \;\Rightarrow\; \sin C = \frac{1}{n} = \frac{1}{1.65} = 0.6061 \]\[ C = \sin^{-1}(0.6061) = 37.3^\circ \]
Za ka so ka ci gaba da wannan aikin?