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Question 1 Report
(a) Define
(i) proton number;
(ii) nucleon number;
(iii) isotopes.
(b) A nuclide \(^A_ZX\) emits \(\beta\)-particle to form a daughter nuclide Y. Write a nuclear equation to illustrate the charge conservation.
(c) The radioactive nuclei \(^{210}_{84}P_o\) emits an \(\alpha\) - particle to produce \(^{206}_{82}P_b\). Calculate the energy, in MeV, released in each disintegration.
Take the masses of \(^{210}_{84}P_o\) = 209.936730 u;
\(^{206}_{82}P_b\) = 205.929421 u;
\(^{4}_{2}He\) = 4.001504 u;
and that 1u = 931 MeV
(a)(i) Proton number (atomic number): the number of protons in the nucleus of an atom.
(ii) Nucleon number (mass number): the total number of protons and neutrons in the nucleus of an atom.
(iii) Isotopes: atoms of the same element that have the same proton number but different nucleon numbers (same number of protons, different numbers of neutrons).
(b) Beta emission converts a neutron into a proton, so the proton number rises by 1 while the nucleon number is unchanged:
\[ {}^{A}_{Z}X \rightarrow {}^{A}_{Z+1}Y + {}^{0}_{-1}e \]Charge conservation: \(Z = (Z+1) + (-1)\), which balances.
(c) Mass defect in the disintegration:
\[ \Delta m = m({}^{210}_{84}Po) - \left[ m({}^{206}_{82}Pb) + m({}^{4}_{2}He) \right] \] \[ \Delta m = 209.936730 - (205.929421 + 4.001504) \] \[ \Delta m = 209.936730 - 209.930925 = 0.005805\ \text{u} \]Energy released:
\[ E = \Delta m \times 931 = 0.005805 \times 931 \] \[ E = 5.40\ \text{MeV} \]The energy released in each disintegration is about \(5.40\ \text{MeV}\).
Answer Details
(a)(i) Proton number (atomic number): the number of protons in the nucleus of an atom.
(ii) Nucleon number (mass number): the total number of protons and neutrons in the nucleus of an atom.
(iii) Isotopes: atoms of the same element that have the same proton number but different nucleon numbers (same number of protons, different numbers of neutrons).
(b) Beta emission converts a neutron into a proton, so the proton number rises by 1 while the nucleon number is unchanged:
\[ {}^{A}_{Z}X \rightarrow {}^{A}_{Z+1}Y + {}^{0}_{-1}e \]Charge conservation: \(Z = (Z+1) + (-1)\), which balances.
(c) Mass defect in the disintegration:
\[ \Delta m = m({}^{210}_{84}Po) - \left[ m({}^{206}_{82}Pb) + m({}^{4}_{2}He) \right] \] \[ \Delta m = 209.936730 - (205.929421 + 4.001504) \] \[ \Delta m = 209.936730 - 209.930925 = 0.005805\ \text{u} \]Energy released:
\[ E = \Delta m \times 931 = 0.005805 \times 931 \] \[ E = 5.40\ \text{MeV} \]The energy released in each disintegration is about \(5.40\ \text{MeV}\).
Question 2 Report
(a) Distinguish between the forces of adhesion and cohension
(b) Give one example each of the forces of adhesion and cohesion.
(a) Adhesion versus cohesion
Adhesive force is the force of attraction between the molecules of two different substances (unlike molecules).
Cohesive force is the force of attraction between the molecules of the same substance (like molecules).
(b) One example each
Answer Details
(a) Adhesion versus cohesion
Adhesive force is the force of attraction between the molecules of two different substances (unlike molecules).
Cohesive force is the force of attraction between the molecules of the same substance (like molecules).
(b) One example each
Question 3 Report
(a)(i) Name and explain the common defects of a primary cell.
(ii) State two advantages of a secondary cell over a primary cell.
(b) Draw a labelled diagram to show the essential parts of a dry leclanche cell.
(c)(i) Explain why six accumulators each of e.m.f 2V connected in series can be used to start the engine of a car whereas eight dry cells each of e.m.f 1.5 V connected in series cannot be used.
(ii) Name the materials used for the positive terminal, the negative terminal and the electrolyte in a
I. leclanche cell;
II. charged lead acid accumulator.
(a)(i) Common defects of a primary (simple) cell:
(a)(ii) Two advantages of a secondary cell over a primary cell:
(b) Labelled diagram of a dry Leclanche cell:
The essential parts are the outer zinc case (negative electrode), the central carbon rod (positive electrode) surrounded by a paste of manganese(IV) oxide and powdered carbon (the depolariser), the ammonium chloride paste (electrolyte), and the pitch/wax seal with a brass cap on top.
(c)(i) The eight dry cells and the six accumulators give the same total e.m.f.: \(8 \times 1.5 = 12\ \text{V}\) and \(6 \times 2 = 12\ \text{V}\). What differs is the internal resistance. A dry (Leclanche) cell has a very high internal resistance, so eight of them in series have a large total internal resistance. When such a battery is connected to the very small resistance of a starter motor, most of the e.m.f. is dropped across the cells' own internal resistance and only a small current \(\left(I = \dfrac{E}{R + r}\right)\) flows, too small to turn the engine. Each accumulator has a very low internal resistance, so six in series can force the very large current needed through the low-resistance starter motor and start the engine.
(c)(ii) Materials used:
| Positive terminal | Negative terminal | Electrolyte | |
| I. Leclanche cell | Carbon rod (surrounded by manganese(IV) oxide, \(\text{MnO}_2\), as depolariser) | Zinc (the case) | Ammonium chloride, \(\text{NH}_4\text{Cl}\) (paste/solution) |
| II. Charged lead-acid accumulator | Lead(IV) oxide, \(\text{PbO}_2\) (lead peroxide) | Spongy lead, \(\text{Pb}\) | Dilute tetraoxosulphate(VI) acid, \(\text{H}_2\text{SO}_4\) (sulphuric acid) |
Answer Details
(a)(i) Common defects of a primary (simple) cell:
(a)(ii) Two advantages of a secondary cell over a primary cell:
(b) Labelled diagram of a dry Leclanche cell:
The essential parts are the outer zinc case (negative electrode), the central carbon rod (positive electrode) surrounded by a paste of manganese(IV) oxide and powdered carbon (the depolariser), the ammonium chloride paste (electrolyte), and the pitch/wax seal with a brass cap on top.
(c)(i) The eight dry cells and the six accumulators give the same total e.m.f.: \(8 \times 1.5 = 12\ \text{V}\) and \(6 \times 2 = 12\ \text{V}\). What differs is the internal resistance. A dry (Leclanche) cell has a very high internal resistance, so eight of them in series have a large total internal resistance. When such a battery is connected to the very small resistance of a starter motor, most of the e.m.f. is dropped across the cells' own internal resistance and only a small current \(\left(I = \dfrac{E}{R + r}\right)\) flows, too small to turn the engine. Each accumulator has a very low internal resistance, so six in series can force the very large current needed through the low-resistance starter motor and start the engine.
(c)(ii) Materials used:
| Positive terminal | Negative terminal | Electrolyte | |
| I. Leclanche cell | Carbon rod (surrounded by manganese(IV) oxide, \(\text{MnO}_2\), as depolariser) | Zinc (the case) | Ammonium chloride, \(\text{NH}_4\text{Cl}\) (paste/solution) |
| II. Charged lead-acid accumulator | Lead(IV) oxide, \(\text{PbO}_2\) (lead peroxide) | Spongy lead, \(\text{Pb}\) | Dilute tetraoxosulphate(VI) acid, \(\text{H}_2\text{SO}_4\) (sulphuric acid) |
Question 4 Report
A paralIel beam of unpolarized light is incident on a plane glass of refractive index 1.60 at an angle to the normal. If the reflected beam is completely polarized, calculate the angle of incidence of the beam.
When the reflected beam is completely (plane) polarised, the angle of incidence equals the polarising angle (Brewster's angle) \(\theta_p\), given by Brewster's law:
\[ n = \tan \theta_p \]Making \(\theta_p\) the subject:
\[ \theta_p = \tan^{-1}(n) = \tan^{-1}(1.60) \] \[ \theta_p = 57.99^{\circ} \approx 58.0^{\circ} \]The angle of incidence of the beam is about \(58^{\circ}\).
Answer Details
When the reflected beam is completely (plane) polarised, the angle of incidence equals the polarising angle (Brewster's angle) \(\theta_p\), given by Brewster's law:
\[ n = \tan \theta_p \]Making \(\theta_p\) the subject:
\[ \theta_p = \tan^{-1}(n) = \tan^{-1}(1.60) \] \[ \theta_p = 57.99^{\circ} \approx 58.0^{\circ} \]The angle of incidence of the beam is about \(58^{\circ}\).
Question 5 Report
(a) With the aid of ray diagrams, explain total internal reflection.
(b) Describe, with the aid of a labelled diagram, the essential features of an astronomical telescope in normal adjustment.
(c) A converging lens forms a real image of a real object. If the magnification is 2 and the distance between the image and the object is 90.0 cm, determine the
(i) focal length of the lens;
(ii) object distance for which the image would be the same size as the object.
(a) Total internal reflection
Total internal reflection occurs when light travels from an optically denser medium to a less dense medium and the angle of incidence is greater than the critical angle, C. At i = C, the angle of refraction is \(90^\circ\), so that the refracted ray travels along the boundary. For \(i>C\), the ray is completely reflected back into the denser medium.
(b) Astronomical telescope in normal adjustment
An astronomical telescope consists of two converging lenses mounted on the same principal axis:
Light from a distant object enters the objective as parallel rays. The objective forms a real, inverted and diminished intermediate image at its principal focus. In normal adjustment, this image is at the first focal point of the eyepiece, so that the principal foci coincide. The eyepiece then produces a final virtual image at infinity, and the emergent rays are parallel.
Hence, for normal adjustment,
\[d=f_o+f_e\]
where \(d\) is the separation of the lenses. The angular magnifying power has magnitude
\[M=\frac{f_o}{f_e}.\]
(c)
For a real image formed by a converging lens,
\[m=\frac{v}{u}=2\]
Therefore,
\[v=2u\]
Since the object and real image are on opposite sides of the lens, their separation is \(u+v\):
\[u+v=90.0\]
\[u+2u=90.0\]
\[3u=90.0\]
\[u=30.0\text{ cm},\qquad v=60.0\text{ cm}.\]
(i) Focal length
Using \(\frac{1}{f}=\frac{1}{u}+\frac{1}{v}\),
\[\frac{1}{f}=\frac{1}{30.0}+\frac{1}{60.0}=\frac{3}{60.0}\]
\[\boxed{f=20.0\text{ cm}}\]
(ii) Object distance for an image of the same size
An image is the same size as the object when the object is at \(2f\).
\[u=2f=2(20.0)=\boxed{40.0\text{ cm}}\]
Answer Details
(a) Total internal reflection
Total internal reflection occurs when light travels from an optically denser medium to a less dense medium and the angle of incidence is greater than the critical angle, C. At i = C, the angle of refraction is \(90^\circ\), so that the refracted ray travels along the boundary. For \(i>C\), the ray is completely reflected back into the denser medium.
(b) Astronomical telescope in normal adjustment
An astronomical telescope consists of two converging lenses mounted on the same principal axis:
Light from a distant object enters the objective as parallel rays. The objective forms a real, inverted and diminished intermediate image at its principal focus. In normal adjustment, this image is at the first focal point of the eyepiece, so that the principal foci coincide. The eyepiece then produces a final virtual image at infinity, and the emergent rays are parallel.
Hence, for normal adjustment,
\[d=f_o+f_e\]
where \(d\) is the separation of the lenses. The angular magnifying power has magnitude
\[M=\frac{f_o}{f_e}.\]
(c)
For a real image formed by a converging lens,
\[m=\frac{v}{u}=2\]
Therefore,
\[v=2u\]
Since the object and real image are on opposite sides of the lens, their separation is \(u+v\):
\[u+v=90.0\]
\[u+2u=90.0\]
\[3u=90.0\]
\[u=30.0\text{ cm},\qquad v=60.0\text{ cm}.\]
(i) Focal length
Using \(\frac{1}{f}=\frac{1}{u}+\frac{1}{v}\),
\[\frac{1}{f}=\frac{1}{30.0}+\frac{1}{60.0}=\frac{3}{60.0}\]
\[\boxed{f=20.0\text{ cm}}\]
(ii) Object distance for an image of the same size
An image is the same size as the object when the object is at \(2f\).
\[u=2f=2(20.0)=\boxed{40.0\text{ cm}}\]
Question 6 Report
The diagram below represents the graph of the force applied in stretching a spiral spring against the corresponding extension produced within its elastic limit.
Using the notations on the graph, determine the:
(a) force constant of the spring;
(b) work done in stretching the spring from 10 x 10\(^{-2}\)m to 20 x 10\(^{-2}\)m.
Within the elastic limit a spiral spring obeys Hooke's law, so the force applied is directly proportional to the extension produced. The force-extension graph is therefore a straight line passing through the origin, as shown below.
Reading the notations on the graph, the line passes through the points: extension \(5\times10^{-2}\) m at force \(15\) N, \(10\times10^{-2}\) m at \(30\) N, \(15\times10^{-2}\) m at \(45\) N, and \(20\times10^{-2}\) m at \(60\) N.
The force constant \(k\) is the slope (gradient) of the force-extension graph:
\[ k = \frac{\Delta F}{\Delta e} = \frac{60 - 0}{(20 - 0)\times10^{-2}} = \frac{60}{20\times10^{-2}} = \frac{60}{0.20} = 300\ \text{N m}^{-1} \]Any point on the line gives the same value, e.g. \(30 / 0.10 = 300\ \text{N m}^{-1}\). Hence the force constant is 300 N m\(^{-1}\).
The work done equals the area under the force-extension graph between the two extensions. From the graph, at \(e_1 = 10\times10^{-2}\) m the force is \(F_1 = 30\) N, and at \(e_2 = 20\times10^{-2}\) m the force is \(F_2 = 60\) N. This shaded region is a trapezium:
\[ W = \tfrac{1}{2}(F_1 + F_2)(e_2 - e_1) = \tfrac{1}{2}(30 + 60)\,(20 - 10)\times10^{-2} \]\[ W = \tfrac{1}{2}(90)(10\times10^{-2}) = \tfrac{1}{2}(90)(0.10) = 4.5\ \text{J} \]Equivalently, using \(W = \tfrac{1}{2}k(e_2^{2} - e_1^{2})\):
\[ W = \tfrac{1}{2}(300)\big[(0.20)^{2} - (0.10)^{2}\big] = 150\,(0.04 - 0.01) = 150 \times 0.03 = 4.5\ \text{J} \]The work done in stretching the spring is 4.5 J.
Answer Details
Within the elastic limit a spiral spring obeys Hooke's law, so the force applied is directly proportional to the extension produced. The force-extension graph is therefore a straight line passing through the origin, as shown below.
Reading the notations on the graph, the line passes through the points: extension \(5\times10^{-2}\) m at force \(15\) N, \(10\times10^{-2}\) m at \(30\) N, \(15\times10^{-2}\) m at \(45\) N, and \(20\times10^{-2}\) m at \(60\) N.
The force constant \(k\) is the slope (gradient) of the force-extension graph:
\[ k = \frac{\Delta F}{\Delta e} = \frac{60 - 0}{(20 - 0)\times10^{-2}} = \frac{60}{20\times10^{-2}} = \frac{60}{0.20} = 300\ \text{N m}^{-1} \]Any point on the line gives the same value, e.g. \(30 / 0.10 = 300\ \text{N m}^{-1}\). Hence the force constant is 300 N m\(^{-1}\).
The work done equals the area under the force-extension graph between the two extensions. From the graph, at \(e_1 = 10\times10^{-2}\) m the force is \(F_1 = 30\) N, and at \(e_2 = 20\times10^{-2}\) m the force is \(F_2 = 60\) N. This shaded region is a trapezium:
\[ W = \tfrac{1}{2}(F_1 + F_2)(e_2 - e_1) = \tfrac{1}{2}(30 + 60)\,(20 - 10)\times10^{-2} \]\[ W = \tfrac{1}{2}(90)(10\times10^{-2}) = \tfrac{1}{2}(90)(0.10) = 4.5\ \text{J} \]Equivalently, using \(W = \tfrac{1}{2}k(e_2^{2} - e_1^{2})\):
\[ W = \tfrac{1}{2}(300)\big[(0.20)^{2} - (0.10)^{2}\big] = 150\,(0.04 - 0.01) = 150 \times 0.03 = 4.5\ \text{J} \]The work done in stretching the spring is 4.5 J.
Question 7 Report
(a) State the conditions for the equilibrium of a rigid body acted upon by parallel forces.
(b)(i) Describe an experiment to determine the mass of a metre rule using the principle of moments.
(ii) State two precautions necessary to obtain accurate results in the experiment described in (b)(i) above.
(c) A bullet of mass 120 g is fired horizontally into a fixed wooden block with a speed of 20 ms\(^{-1}\). If the bullet is brought to rest in the block in 0.1s by a constant resistance, calculate the (i) magnitude of the resistance; (ii) distance moved by the bullet in the wood.
(a) Conditions for equilibrium under parallel forces:
(b)(i) Experiment to find the mass of a metre rule: Suspend the metre rule from a knife-edge and find its centre of gravity \(G\) (the balance point with no load). Hang a known mass \(m\) at a distance \(d_1\) on one side of a chosen pivot, and adjust the position of the pivot until the rule balances horizontally. Measure the distance \(d_2\) from the pivot to \(G\) (through which the whole weight \(W = Mg\) of the rule acts). Taking moments about the pivot:
\[ m g \times d_1 = M g \times d_2 \Rightarrow M = \frac{m \, d_1}{d_2} \]which gives the mass \(M\) of the rule.
(ii) Two precautions:
(c) Bullet mass \(m = 120\ \text{g} = 0.12\ \text{kg}\), \(u = 20\ \text{ms}^{-1}\), \(v = 0\), \(t = 0.1\ \text{s}\).
(i) Resistance (retarding force):
\[ F = \frac{m(u - v)}{t} = \frac{0.12 \times (20 - 0)}{0.1} = \frac{2.4}{0.1} = 24\ \text{N} \](ii) Distance moved in the wood (average velocity method):
\[ s = \left(\frac{u + v}{2}\right) t = \left(\frac{20 + 0}{2}\right) \times 0.1 = 10 \times 0.1 = 1.0\ \text{m} \]The resistance is \(24\ \text{N}\) and the bullet travels \(1.0\ \text{m}\) into the block.
Answer Details
(a) Conditions for equilibrium under parallel forces:
(b)(i) Experiment to find the mass of a metre rule: Suspend the metre rule from a knife-edge and find its centre of gravity \(G\) (the balance point with no load). Hang a known mass \(m\) at a distance \(d_1\) on one side of a chosen pivot, and adjust the position of the pivot until the rule balances horizontally. Measure the distance \(d_2\) from the pivot to \(G\) (through which the whole weight \(W = Mg\) of the rule acts). Taking moments about the pivot:
\[ m g \times d_1 = M g \times d_2 \Rightarrow M = \frac{m \, d_1}{d_2} \]which gives the mass \(M\) of the rule.
(ii) Two precautions:
(c) Bullet mass \(m = 120\ \text{g} = 0.12\ \text{kg}\), \(u = 20\ \text{ms}^{-1}\), \(v = 0\), \(t = 0.1\ \text{s}\).
(i) Resistance (retarding force):
\[ F = \frac{m(u - v)}{t} = \frac{0.12 \times (20 - 0)}{0.1} = \frac{2.4}{0.1} = 24\ \text{N} \](ii) Distance moved in the wood (average velocity method):
\[ s = \left(\frac{u + v}{2}\right) t = \left(\frac{20 + 0}{2}\right) \times 0.1 = 10 \times 0.1 = 1.0\ \text{m} \]The resistance is \(24\ \text{N}\) and the bullet travels \(1.0\ \text{m}\) into the block.
Question 8 Report
(a) State two;
(i) laws of solid friction;
(ii) advantages of friction;
(iii) methods of reducing friction.
(b) Draw and label a diagram of a pulley system with velocity ratio of 5.
(c)(i) Show that the efficiency L, force ratio M.A. and the velocity ratio V.R. of a machine are related by the equation \(E = \frac{M.A.}{V.R}\) x 100%.
(ii) The efficiency of a machine is 80%. Calcuate the work done by a person using the machine to raise a load of 300 kg through a height of 4 m.[ g = 10 ms\(^{-2}\) ]
(a)(i) Two laws of solid friction:
(a)(ii) Two advantages of friction:
(a)(iii) Two methods of reducing friction:
(b) Pulley system with velocity ratio of 5:
A block-and-tackle whose velocity ratio is 5 has five rope segments (strings) supporting the movable (lower) block. This is arranged with 3 pulleys in the fixed upper block and 2 pulleys in the movable lower block. The load \(W\) hangs from the lower block and the effort \(E\) is applied to the free end of the rope.
Because 5 strings support the lower block, when the effort end is pulled through a distance of 5 units the load rises through only 1 unit, giving
\[ \text{V.R.} = \frac{\text{distance moved by effort}}{\text{distance moved by load}} = \frac{5}{1} = 5. \]
(c)(i) Relationship between efficiency, mechanical advantage and velocity ratio:
Efficiency is the ratio of useful work output to work input, expressed as a percentage:
\[ E = \frac{\text{work output}}{\text{work input}} \times 100\% = \frac{\text{load} \times \text{distance moved by load}}{\text{effort} \times \text{distance moved by effort}} \times 100\%. \]
Rearranging the factors,
\[ E = \left(\frac{\text{load}}{\text{effort}}\right) \times \left(\frac{\text{distance moved by load}}{\text{distance moved by effort}}\right) \times 100\%. \]
Now \(\dfrac{\text{load}}{\text{effort}} = \text{M.A.}\) and \(\dfrac{\text{distance moved by effort}}{\text{distance moved by load}} = \text{V.R.}\), so \(\dfrac{\text{distance moved by load}}{\text{distance moved by effort}} = \dfrac{1}{\text{V.R.}}\). Therefore
\[ E = \frac{\text{M.A.}}{\text{V.R.}} \times 100\%. \]
(c)(ii) Work done by the person (work input):
Useful work output in raising the load:
\[ W_{\text{out}} = mgh = 300 \times 10 \times 4 = 12000\ \text{J}. \]
Since efficiency \(E = \dfrac{W_{\text{out}}}{W_{\text{in}}} \times 100\%\), the work input (work done by the person) is
\[ W_{\text{in}} = \frac{W_{\text{out}}}{E} = \frac{12000}{0.80} = 15000\ \text{J}. \]
The work done by the person is \(W_{\text{in}} = 15000\ \text{J} = 15\ \text{kJ}\).
Answer Details
(a)(i) Two laws of solid friction:
(a)(ii) Two advantages of friction:
(a)(iii) Two methods of reducing friction:
(b) Pulley system with velocity ratio of 5:
A block-and-tackle whose velocity ratio is 5 has five rope segments (strings) supporting the movable (lower) block. This is arranged with 3 pulleys in the fixed upper block and 2 pulleys in the movable lower block. The load \(W\) hangs from the lower block and the effort \(E\) is applied to the free end of the rope.
Because 5 strings support the lower block, when the effort end is pulled through a distance of 5 units the load rises through only 1 unit, giving
\[ \text{V.R.} = \frac{\text{distance moved by effort}}{\text{distance moved by load}} = \frac{5}{1} = 5. \]
(c)(i) Relationship between efficiency, mechanical advantage and velocity ratio:
Efficiency is the ratio of useful work output to work input, expressed as a percentage:
\[ E = \frac{\text{work output}}{\text{work input}} \times 100\% = \frac{\text{load} \times \text{distance moved by load}}{\text{effort} \times \text{distance moved by effort}} \times 100\%. \]
Rearranging the factors,
\[ E = \left(\frac{\text{load}}{\text{effort}}\right) \times \left(\frac{\text{distance moved by load}}{\text{distance moved by effort}}\right) \times 100\%. \]
Now \(\dfrac{\text{load}}{\text{effort}} = \text{M.A.}\) and \(\dfrac{\text{distance moved by effort}}{\text{distance moved by load}} = \text{V.R.}\), so \(\dfrac{\text{distance moved by load}}{\text{distance moved by effort}} = \dfrac{1}{\text{V.R.}}\). Therefore
\[ E = \frac{\text{M.A.}}{\text{V.R.}} \times 100\%. \]
(c)(ii) Work done by the person (work input):
Useful work output in raising the load:
\[ W_{\text{out}} = mgh = 300 \times 10 \times 4 = 12000\ \text{J}. \]
Since efficiency \(E = \dfrac{W_{\text{out}}}{W_{\text{in}}} \times 100\%\), the work input (work done by the person) is
\[ W_{\text{in}} = \frac{W_{\text{out}}}{E} = \frac{12000}{0.80} = 15000\ \text{J}. \]
The work done by the person is \(W_{\text{in}} = 15000\ \text{J} = 15\ \text{kJ}\).
Question 9 Report
Explain why water in a narrow glass tube has a concave meniscus while mecury in the same tube, has a convex meniscus
Shape of the meniscus: water versus mercury
The shape of the meniscus depends on the relative strengths of the adhesive force (attraction between the liquid and the glass) and the cohesive force (attraction between the liquid molecules themselves).
Water (concave meniscus): for water in glass, the adhesive force between water and glass is greater than the cohesive force between the water molecules. The water therefore wets the glass and is pulled up the walls, so the surface curves upward at the edges, giving a concave (curving-down in the middle) meniscus.
Mercury (convex meniscus): for mercury in glass, the cohesive force between mercury molecules is much greater than the adhesive force between mercury and glass. The mercury does not wet the glass; its molecules are pulled together and away from the walls, so the surface is depressed at the edges and bulges up in the middle, giving a convex meniscus.
Answer Details
Shape of the meniscus: water versus mercury
The shape of the meniscus depends on the relative strengths of the adhesive force (attraction between the liquid and the glass) and the cohesive force (attraction between the liquid molecules themselves).
Water (concave meniscus): for water in glass, the adhesive force between water and glass is greater than the cohesive force between the water molecules. The water therefore wets the glass and is pulled up the walls, so the surface curves upward at the edges, giving a concave (curving-down in the middle) meniscus.
Mercury (convex meniscus): for mercury in glass, the cohesive force between mercury molecules is much greater than the adhesive force between mercury and glass. The mercury does not wet the glass; its molecules are pulled together and away from the walls, so the surface is depressed at the edges and bulges up in the middle, giving a convex meniscus.
Question 10 Report
The uncertinty in determining the duration during which an electron remains in a particular energy level before returning to the ground state is 2.0 x 10\(^{-9}\)s. Calculate the uncertainty in determining its energy at that level [Take \(\frac{h}{2\pi} = h = 1.054 \times 10^{-34}\) Js]
\(\Delta E \Delta t \geq \dfrac{h}{2\pi}\)
\(\Delta E \geq \dfrac{h/2\pi}{\Delta t}\)
\(\Delta E \geq \dfrac{1.054 \times 10^{-34}}{2.0 \times 10^{-9}}\)
\(\Delta E \geq 5.27 \times 10^{-26}\ \text{J}\)
Answer Details
\(\Delta E \Delta t \geq \dfrac{h}{2\pi}\)
\(\Delta E \geq \dfrac{h/2\pi}{\Delta t}\)
\(\Delta E \geq \dfrac{1.054 \times 10^{-34}}{2.0 \times 10^{-9}}\)
\(\Delta E \geq 5.27 \times 10^{-26}\ \text{J}\)
Question 11 Report
A particle dropped from a vertical height and falls freely for a time interval t. Sketch and explain a graph to show how h varies with (a) t (b) t\(^{2}\).
Take h as the height of the particle above the ground and let it be released from rest from a height H. Since the fall is free (only gravity acts), the distance fallen after time t is \(\tfrac{1}{2}gt^{2}\), so the height still remaining above the ground is
\n\[ h = H - \tfrac{1}{2}\,g\,t^{2}. \]
\nUsing \(H = 45\ \text{m}\) and \(g = 10\ \text{m s}^{-2}\) as a worked illustration, \(h = 45 - 5t^{2}\). The values are:
\n| t /s | 0 | 0.5 | 1.0 | 1.5 | 2.0 | 2.5 | 3.0 |
| t\(^{2}\) /s\(^{2}\) | 0 | 0.25 | 1.0 | 2.25 | 4.0 | 6.25 | 9.0 |
| h /m | 45 | 43.75 | 40 | 33.75 | 25 | 13.75 | 0 |
Because \(h = H - \tfrac{1}{2}gt^{2}\), the term subtracted grows as the square of the time. The graph therefore starts at \(h = H\) on the vertical axis and curves downward (a parabola, concave down). Its slope, which is the negative of the speed \(\left(\dfrac{dh}{dt} = -gt\right)\), is zero at the instant of release and becomes steadily steeper as the particle accelerates, reaching the ground (\(h = 0\)) after \(t = 3\ \text{s}\). So h falls slowly at first and ever faster afterwards, giving a curved (non-linear) graph.
\nWriting \(x = t^{2}\), the relation becomes \(h = H - \tfrac{1}{2}g\,x\), which is of the linear form \(y = c + mx\). The graph of h against \(t^{2}\) is therefore a straight line with
\nReading the slope from the line, \[ \text{slope} = \frac{0 - 45}{9 - 0} = -5\ \text{m s}^{-2} = -\tfrac{1}{2}g, \] which gives \(g = 10\ \text{m s}^{-2}\). Thus plotting h against \(t^{2}\) straightens the curve of part (a) into a line whose gradient conveniently yields the acceleration due to gravity.
Answer Details
Take h as the height of the particle above the ground and let it be released from rest from a height H. Since the fall is free (only gravity acts), the distance fallen after time t is \(\tfrac{1}{2}gt^{2}\), so the height still remaining above the ground is
\n\[ h = H - \tfrac{1}{2}\,g\,t^{2}. \]
\nUsing \(H = 45\ \text{m}\) and \(g = 10\ \text{m s}^{-2}\) as a worked illustration, \(h = 45 - 5t^{2}\). The values are:
\n| t /s | 0 | 0.5 | 1.0 | 1.5 | 2.0 | 2.5 | 3.0 |
| t\(^{2}\) /s\(^{2}\) | 0 | 0.25 | 1.0 | 2.25 | 4.0 | 6.25 | 9.0 |
| h /m | 45 | 43.75 | 40 | 33.75 | 25 | 13.75 | 0 |
Because \(h = H - \tfrac{1}{2}gt^{2}\), the term subtracted grows as the square of the time. The graph therefore starts at \(h = H\) on the vertical axis and curves downward (a parabola, concave down). Its slope, which is the negative of the speed \(\left(\dfrac{dh}{dt} = -gt\right)\), is zero at the instant of release and becomes steadily steeper as the particle accelerates, reaching the ground (\(h = 0\)) after \(t = 3\ \text{s}\). So h falls slowly at first and ever faster afterwards, giving a curved (non-linear) graph.
\nWriting \(x = t^{2}\), the relation becomes \(h = H - \tfrac{1}{2}g\,x\), which is of the linear form \(y = c + mx\). The graph of h against \(t^{2}\) is therefore a straight line with
\nReading the slope from the line, \[ \text{slope} = \frac{0 - 45}{9 - 0} = -5\ \text{m s}^{-2} = -\tfrac{1}{2}g, \] which gives \(g = 10\ \text{m s}^{-2}\). Thus plotting h against \(t^{2}\) straightens the curve of part (a) into a line whose gradient conveniently yields the acceleration due to gravity.
Question 12 Report
(a) State two applications of electrolysis.
(b) Explain what is meant by the electrochemical equivalent of copper is 3.3 x 10\(^{-7}\) kgC\(^{-1}\)
(a) Two applications of electrolysis
(Other acceptable uses: extraction of reactive metals like aluminium; electrotyping; production of chemicals such as chlorine and caustic soda.)
(b) Meaning of "the electrochemical equivalent of copper is \(3.3\times10^{-7}\ \text{kg C}^{-1}\)"
The electrochemical equivalent (\(z\)) of copper is the mass of copper deposited (or liberated) by a charge of one coulomb during electrolysis. So the statement means that a charge of 1 coulomb passing through a copper solution deposits \(3.3\times10^{-7}\ \text{kg}\) of copper. From Faraday's first law, \(m = z\,It\), where \(I\) is the current and \(t\) the time.
Answer Details
(a) Two applications of electrolysis
(Other acceptable uses: extraction of reactive metals like aluminium; electrotyping; production of chemicals such as chlorine and caustic soda.)
(b) Meaning of "the electrochemical equivalent of copper is \(3.3\times10^{-7}\ \text{kg C}^{-1}\)"
The electrochemical equivalent (\(z\)) of copper is the mass of copper deposited (or liberated) by a charge of one coulomb during electrolysis. So the statement means that a charge of 1 coulomb passing through a copper solution deposits \(3.3\times10^{-7}\ \text{kg}\) of copper. From Faraday's first law, \(m = z\,It\), where \(I\) is the current and \(t\) the time.
Question 13 Report
A particle is projected horizontally at 10 ms\(^{-1}\) from a height of 45m. Calculate the horizontal distance covered by the particle before hitting the ground. [g = 10ms\(^{-1}\)]
Horizontal projectile
Horizontal velocity \(u = 10\ \text{m s}^{-1}\), height \(h = 45\ \text{m}\), \(g = 10\ \text{m s}^{-2}\).
Time to fall (vertical motion, initial vertical velocity zero):
\(h = \tfrac{1}{2}g t^{2} \Rightarrow 45 = \tfrac{1}{2}\times10\times t^{2} = 5t^{2}\).
\(t^{2} = 9 \Rightarrow t = 3\ \text{s}\).
Horizontal distance (range): \(R = u\,t = 10\times3 = 30\ \text{m}\).
The particle covers a horizontal distance of 30 m before hitting the ground.
Answer Details
Horizontal projectile
Horizontal velocity \(u = 10\ \text{m s}^{-1}\), height \(h = 45\ \text{m}\), \(g = 10\ \text{m s}^{-2}\).
Time to fall (vertical motion, initial vertical velocity zero):
\(h = \tfrac{1}{2}g t^{2} \Rightarrow 45 = \tfrac{1}{2}\times10\times t^{2} = 5t^{2}\).
\(t^{2} = 9 \Rightarrow t = 3\ \text{s}\).
Horizontal distance (range): \(R = u\,t = 10\times3 = 30\ \text{m}\).
The particle covers a horizontal distance of 30 m before hitting the ground.
Question 14 Report
(a) Explain the statement the acceleration of free fall cohesion.
(b) State two factors that can affect the value of the narrow glass tube has a concave meniscus while acceleration of free fall at a place.
The OCR text of this question is partly garbled; the coherent physics content is about the acceleration of free fall, answered below.
(a) Meaning of "the acceleration of free fall at a place is \(9.8\ \text{m s}^{-2}\)"
It means that a body falling freely under gravity alone (with no air resistance) at that place has its velocity increasing at a constant rate of \(9.8\ \text{metres per second every second}\); that is, each second its downward speed increases by \(9.8\ \text{m s}^{-1}\).
(b) Two factors that affect the value of the acceleration of free fall at a place
Answer Details
The OCR text of this question is partly garbled; the coherent physics content is about the acceleration of free fall, answered below.
(a) Meaning of "the acceleration of free fall at a place is \(9.8\ \text{m s}^{-2}\)"
It means that a body falling freely under gravity alone (with no air resistance) at that place has its velocity increasing at a constant rate of \(9.8\ \text{metres per second every second}\); that is, each second its downward speed increases by \(9.8\ \text{m s}^{-1}\).
(b) Two factors that affect the value of the acceleration of free fall at a place
Question 15 Report
List three observations in support of the de-Broglie's assumptions that moving particles behave like waves.
Three observations supporting de Broglie’s assumption that moving particles behave like waves are:
Answer Details
Three observations supporting de Broglie’s assumption that moving particles behave like waves are:
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