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Question 7761Question

In Bohr's atomic model of the hydrogen atom, the radius of the ground state orbit (n=1n = 1) is 0.053 nm0.053\text{ nm}. According to de Broglie's condition for stationary electron orbits, what is the de Broglie wavelength of the electron in its second excited state? Express your answer in nanometers (nm\text{nm}).

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Answer: 1

Answer

The de Broglie wavelength of the electron in its second excited state is 1.00 nm1.00\text{ nm}.
The second excited state corresponds to the quantum number n=3n = 3. According to Bohr's atomic model, the radius of the nn-th orbit is given by rn=n2r1r_n = n^2 r_1, yielding r3=32×0.053 nm=0.477 nmr_3 = 3^2 \times 0.053\text{ nm} = 0.477\text{ nm}. De Broglie explained Bohr's angular momentum quantization by showing that an integral number of electron matter-waves must fit around the orbital circumference: 2πrn=nλn2\pi r_n = n \lambda_n. Solving for λ3\lambda_3 gives λ3=2πr33=2π×3×0.053 nm1.00 nm\lambda_3 = \frac{2\pi r_3}{3} = 2\pi \times 3 \times 0.053\text{ nm} \approx 1.00\text{ nm}.

Step-by-Step Solution

1
Identify the principal quantum number for the specified energy state
n=3n = 3
The ground state corresponds to n=1n = 1, the first excited state to n=2n = 2, and the second excited state to n=3n = 3.
2
Calculate the radius of the third stationary orbit
r3=0.477 nmr_3 = 0.477\text{ nm}
In Bohr's model, the radius of the nn-th orbit is proportional to n2n^2, so r3=32×0.053 nm=9×0.053 nm=0.477 nmr_3 = 3^2 \times 0.053\text{ nm} = 9 \times 0.053\text{ nm} = 0.477\text{ nm}.
3
Apply de Broglie's standing wave condition for stationary orbits
λ3=2πr33\lambda_3 = \frac{2\pi r_3}{3}
De Broglie postulated that a stationary orbit contains an integral number of electron de Broglie wavelengths around its circumference: 2πrn=nλn2\pi r_n = n \lambda_n.
4
Substitute values to compute the wavelength
λ3=1.00 nm\lambda_3 = 1.00\text{ nm}
λ3=2×3.1416×0.477 nm3=2π×3×0.053 nm0.9992 nm1.00 nm\lambda_3 = \frac{2 \times 3.1416 \times 0.477\text{ nm}}{3} = 2\pi \times 3 \times 0.053\text{ nm} \approx 0.9992\text{ nm} \approx 1.00\text{ nm}.

Key Concept

De Broglie Standing Wave Quantization in Bohr Atomic Model
Question 7762Question

A ray of light traveling inside a transparent medium strikes the boundary with air. If the critical angle for total internal reflection at this boundary is 3030^\circ, what is the refractive index of the medium?

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Answer: 2.002.00

Answer

The refractive index of the medium is 2.002.00.
For light traveling from a medium into air, the critical angle CC is related to the refractive index nn by n=1sinCn = \frac{1}{\sin C}. Substituting C=30C = 30^\circ gives n=1sin30=10.5=2.00n = \frac{1}{\sin 30^\circ} = \frac{1}{0.5} = 2.00.

Step-by-Step Solution

1
Identify the relationship between critical angle CC and refractive index nn
The formula for light passing into air is n=1sinCn = \frac{1}{\sin C}.
Total internal reflection occurs when light travels from a denser medium to a less dense medium (air, nair=1n_{air} = 1) at an angle greater than the critical angle.
2
Substitute the given critical angle C=30C = 30^\circ into the formula
sin30=0.5\sin 30^\circ = 0.5, so n=10.5=2.00n = \frac{1}{0.5} = 2.00.
Taking the reciprocal of sin30\sin 30^\circ gives the correct refractive index.

Key Concept

Critical Angle and Refractive Index
Question 7763Question

The pressure PP of a given mass of gas varies directly as its absolute temperature TT and inversely as its volume VV. Given that P=50 kPaP = 50\text{ kPa} when T=300 KT = 300\text{ K} and V=10 m3V = 10\text{ m}^3, what is the value of PP when T=360 KT = 360\text{ K} and V=8 m3V = 8\text{ m}^3?

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Answer: 75 kPa75\text{ kPa}

Answer

75 kPa75\text{ kPa}
The relationship is governed by P=kTVP = \frac{kT}{V}. Substituting P=50P = 50, T=300T = 300, and V=10V = 10 yields k=53k = \frac{5}{3}. Using k=53k = \frac{5}{3} with T=360T = 360 and V=8V = 8 gives P=(5/3)×3608=75 kPaP = \frac{(5/3) \times 360}{8} = 75\text{ kPa}.

Step-by-Step Solution

1
Set up the general formula for joint and inverse variation.
P=kTVP = \frac{kT}{V}, where kk is the constant of variation.
Pressure varies directly as temperature TT and inversely as volume VV.
2
Substitute initial conditions to determine kk.
50=k×30010    50=30k    k=5350 = \frac{k \times 300}{10} \implies 50 = 30k \implies k = \frac{5}{3}.
The initial values P=50 kPaP = 50\text{ kPa}, T=300 KT = 300\text{ K}, and V=10 m3V = 10\text{ m}^3 allow solving for kk.
3
Calculate the new pressure with updated temperature and volume values.
P=53×3608=6008=75 kPaP = \frac{\frac{5}{3} \times 360}{8} = \frac{600}{8} = 75\text{ kPa}.
Substitute k=53k = \frac{5}{3}, T=360 KT = 360\text{ K}, and V=8 m3V = 8\text{ m}^3 into the variation formula.

Key Concept

Joint and inverse variation in algebraic relationships
Estimated Time:1m 30s
Question 7764Question

Let AA be a 3×33 \times 3 square matrix such that det(A)>0\det(A) > 0. If the matrix satisfies the property det(3A1)=det(ATA)\det(3A^{-1}) = \det(A^T A), what is the value of det(A)\det(A)?

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Answer: 3

Answer

The value of det(A)\det(A) is 3.
Using fundamental determinant identities for a 3×33 \times 3 matrix (n=3n = 3): det(3A1)=33det(A1)=27det(A)\det(3A^{-1}) = 3^3 \det(A^{-1}) = \frac{27}{\det(A)} and det(ATA)=det(AT)det(A)=(det(A))2\det(A^T A) = \det(A^T)\det(A) = (\det(A))^2. Equating them yields 27det(A)=(det(A))2    (det(A))3=27\frac{27}{\det(A)} = (\det(A))^2 \implies (\det(A))^3 = 27, which yields det(A)=3\det(A) = 3.

Step-by-Step Solution

1
Express det(3A1)\det(3A^{-1}) in terms of det(A)\det(A) using determinant scaling and inverse properties.
\det(3A^{-1}) = 3^3 \det(A^{-1}) = \frac{27}{\det(A)}.
For an n×nn \times n matrix MM, scaling by constant kk gives det(kM)=kndet(M)\det(kM) = k^n \det(M), and det(M1)=1det(M)\det(M^{-1}) = \frac{1}{\det(M)}.
2
Express det(ATA)\det(A^T A) in terms of det(A)\det(A) using transpose and multiplication properties.
\det(A^T A) = \det(A^T)\det(A) = (\det(A))^2.
The determinant of a product is the product of determinants, and det(AT)=det(A)\det(A^T) = \det(A).
3
Set the two simplified expressions equal to each other and solve for det(A)\det(A).
\frac{27}{\det(A)} = (\det(A))^2 \implies (\det(A))^3 = 27 \implies \det(A) = 3.
Taking the cube root of both sides gives the unique real value since det(A)>0\det(A) > 0.

Key Concept

Properties of Determinants (Scalar Multiplication, Transpose, Inverse, and Matrix Products)
Estimated Time:1m 30s
Question 7765Question

Three capacitors, each of capacitance 12 μF12\text{ }\mu\text{F}, are arranged such that two of them are connected in parallel, and this combination is connected in series with the third capacitor. If the entire network is connected across a 20 V20\text{ V} d.c. power supply, what is the total energy stored in the network?

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Answer: 1.6×103 J1.6 \times 10^{-3}\text{ J}

Answer

The total energy stored in the network is 1.6×103 J1.6 \times 10^{-3}\text{ J}.
Combining two 12 μF12\text{ }\mu\text{F} capacitors in parallel gives a parallel capacitance of 24 μF24\text{ }\mu\text{F}. Connecting this combination in series with the third 12 μF12\text{ }\mu\text{F} capacitor results in an equivalent network capacitance of Ceq=24×1224+12=8 μFC_{\text{eq}} = \frac{24 \times 12}{24 + 12} = 8\text{ }\mu\text{F}. Substituting this into the energy formula E=12CeqV2E = \frac{1}{2} C_{\text{eq}} V^2 yields E=12×8×106×400=1.6×103 JE = \frac{1}{2} \times 8 \times 10^{-6} \times 400 = 1.6 \times 10^{-3}\text{ J}.

Step-by-Step Solution

1
Calculate the equivalent capacitance of the parallel branch.
Cp=12 μF+12 μF=24 μFC_p = 12\text{ }\mu\text{F} + 12\text{ }\mu\text{F} = 24\text{ }\mu\text{F}
Capacitors in parallel add directly.
2
Calculate the total equivalent capacitance of the network.
Ceq=Cp×C3Cp+C3=24×1224+12=28836=8 μF=8×106 FC_{\text{eq}} = \frac{C_p \times C_3}{C_p + C_3} = \frac{24 \times 12}{24 + 12} = \frac{288}{36} = 8\text{ }\mu\text{F} = 8 \times 10^{-6}\text{ F}
The parallel combination is connected in series with the third capacitor.
3
Calculate the total electrical energy stored in the combination.
E=12CeqV2=12×(8×106 F)×(20 V)2=4×106×400=1.6×103 JE = \frac{1}{2} C_{\text{eq}} V^2 = \frac{1}{2} \times (8 \times 10^{-6}\text{ F}) \times (20\text{ V})^2 = 4 \times 10^{-6} \times 400 = 1.6 \times 10^{-3}\text{ J}
The formula for energy stored in a capacitor network is E=12CV2E = \frac{1}{2} C V^2.

Key Concept

Mixed capacitor networks and energy storage
Estimated Time:1m 30s
Question 7766Question

An electric train accelerates uniformly from rest at a rate of 2 m/s22\text{ m/s}^2 and then immediately decelerates uniformly at 4 m/s24\text{ m/s}^2 until it comes to a complete stop. If the total distance covered by the train during this entire motion is 600 m600\text{ m}, what is the total time taken for the journey?

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Answer: 30 s30\text{ s}

Answer

The total time taken for the journey is 30 s30\text{ s}.
For motion from rest back to rest, the velocity-time graph forms a triangle of total base TT and height vmaxv_{\text{max}}. Acceleration time is t1=vmax/2t_1 = v_{\text{max}}/2 and deceleration time is t2=vmax/4=0.5t1t_2 = v_{\text{max}}/4 = 0.5 t_1. The total displacement is s=12(2)t12+12(4)t22=t12+2(0.5t1)2=1.5t12=600 ms = \frac{1}{2} (2) t_1^2 + \frac{1}{2} (4) t_2^2 = t_1^2 + 2 (0.5 t_1)^2 = 1.5 t_1^2 = 600\text{ m}, yielding t1=20 st_1 = 20\text{ s} and t2=10 st_2 = 10\text{ s}. Summing these gives a total journey time of 30 s30\text{ s}.

Step-by-Step Solution

1
Relate maximum velocity to time in each stage.
Let vmaxv_{\text{max}} be the maximum velocity. Acceleration time t1=vmax2t_1 = \frac{v_{\text{max}}}{2} and deceleration time t2=vmax4t_2 = \frac{v_{\text{max}}}{4}.
Using v=u+atv = u + at from rest to vmaxv_{\text{max}} and from vmaxv_{\text{max}} to rest.
2
Express total time TT in terms of maximum velocity.
T=t1+t2=vmax2+vmax4=34vmaxT = t_1 + t_2 = \frac{v_{\text{max}}}{2} + \frac{v_{\text{max}}}{4} = \frac{3}{4} v_{\text{max}}, which gives vmax=43Tv_{\text{max}} = \frac{4}{3} T.
Total duration is the sum of individual phase durations.
3
Set up distance equation from the area of the velocity-time graph.
\text{Total distance } s = \frac{1}{2} \times T \times v_{\text{max}} = \frac{1}{2} \times T \times \frac{4}{3} T = \frac{2}{3} T^2 = 600\text{ m}.
Area under a velocity-time triangle equals total displacement.
4
Solve for total time TT.
T2=600×32=900    T=30 sT^2 = 600 \times \frac{3}{2} = 900 \implies T = 30\text{ s}.
Taking the square root gives the total travel time.

Key Concept

Multi-stage linear motion with uniform acceleration and deceleration
Question 7767Question

Two electrostatic forces of magnitude 3.0 N3.0\text{ N} and 4.0 N4.0\text{ N} act on a small test charge at right angles (9090^\circ) to each other. What is the magnitude of the net electrostatic force acting on the charge?

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Answer: 5.0 N5.0\text{ N}

Answer

5.0 N5.0\text{ N}
The net electrostatic force is found by vector addition. Since the two forces are perpendicular (9090^\circ), the magnitude of their resultant is given by F12+F22=3.02+4.02=5.0 N\sqrt{F_1^2 + F_2^2} = \sqrt{3.0^2 + 4.0^2} = 5.0\text{ N}.

Step-by-Step Solution

1
Identify the nature of force as a vector quantity.
Electrostatic forces must be combined using vector addition rather than simple scalar addition.
The forces act at right angles (9090^\circ) to each other.
2
Apply the Pythagorean theorem to calculate the magnitude of the resultant net force FnetF_{\text{net}}.
Fnet=F12+F22=3.02+4.02=9+16=25=5.0 NF_{\text{net}} = \sqrt{F_1^2 + F_2^2} = \sqrt{3.0^2 + 4.0^2} = \sqrt{9 + 16} = \sqrt{25} = 5.0\text{ N}.
For perpendicular vectors, the resultant is the hypotenuse of a right-angled triangle formed by the vector components.

Key Concept

Vector Addition of Electrostatic Forces
Question 7768Question

Match each statistical chart term or parameter in Column A with its corresponding definition or formula in Column B.

Click a left item, then click its matching right item

Items

Class boundary
Frequency density
Cumulative frequency
Pie chart sector angle

Matches

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Answer

Class boundary matches the exact continuous limit of a class interval; Frequency density matches the quotient of class frequency and class width; Cumulative frequency matches the running total of frequencies plotted on an ogive; Pie chart sector angle matches the central angle formula involving multiplication by 360 degrees.
Each chart parameter in Column A directly corresponds to its standard mathematical definition, formula, or geometric representation in Column B.

Step-by-Step Solution

1
Identify the statistical definition for continuous class intervals in histograms.
Class boundaries remove gaps between non-overlapping class limits.
Histograms require continuous real class boundaries on the horizontal axis.
2
Recall the formula for histogram bar height when class intervals vary.
Frequency density = FrequencyClass Width\frac{\text{Frequency}}{\text{Class Width}}.
Bar area must remain proportional to frequency.
3
Determine the parameter used to plot an ogive curve.
Cumulative frequency tracks accumulated totals across upper class boundaries.
An ogive represents cumulative distribution.
4
Identify the angular calculation for circular charts.
Sector angle = Class FrequencyTotal Frequency×360\frac{\text{Class Frequency}}{\text{Total Frequency}} \times 360^\circ.
A complete pie chart represents 360 degrees.

Key Concept

Data Representation and Chart Properties
Question 7769Question

Given that (x3)(x - 3) is a factor of the polynomial P(x)=x3+kx2+mx6P(x) = x^3 + kx^2 + mx - 6 and that dividing P(x)P(x) by (x+1)(x + 1) leaves a remainder of 12-12, what is the value of k+mk + m?

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Answer: 1-1

Answer

The value of k+mk + m is 1-1.
Applying the Factor Theorem P(3)=0P(3) = 0 gives 3k+m=73k + m = -7, and applying the Remainder Theorem P(1)=12P(-1) = -12 gives km=5k - m = -5. Solving these simultaneous linear equations gives k=3k = -3 and m=2m = 2, which sums to k+m=1k + m = -1.

Step-by-Step Solution

1
Apply the Factor Theorem for the linear factor (x3)(x - 3)
3k+m=73k + m = -7
By the Factor Theorem, if (x3)(x - 3) is a factor, then P(3)=0P(3) = 0. Substituting x=3x = 3 gives 33+k(3)2+m(3)6=0    27+9k+3m6=0    9k+3m=21    3k+m=73^3 + k(3)^2 + m(3) - 6 = 0 \implies 27 + 9k + 3m - 6 = 0 \implies 9k + 3m = -21 \implies 3k + m = -7.
2
Apply the Remainder Theorem for the divisor (x+1)(x + 1)
km=5k - m = -5
By the Remainder Theorem, dividing P(x)P(x) by (x+1)(x + 1) gives remainder P(1)=12P(-1) = -12. Substituting x=1x = -1 gives (1)3+k(1)2+m(1)6=12    1+km6=12    km7=12    km=5(-1)^3 + k(-1)^2 + m(-1) - 6 = -12 \implies -1 + k - m - 6 = -12 \implies k - m - 7 = -12 \implies k - m = -5.
3
Solve the system of linear equations for kk and mm
k=3k = -3 and m=2m = 2
Adding the two equations (3k+m)+(km)=7+(5)(3k + m) + (k - m) = -7 + (-5) gives 4k=12    k=34k = -12 \implies k = -3. Substituting k=3k = -3 into km=5k - m = -5 gives 3m=5    m=2-3 - m = -5 \implies m = 2.
4
Calculate the target value k+mk + m
k+m=1k + m = -1
Summing k=3k = -3 and m=2m = 2 yields k+m=3+2=1k + m = -3 + 2 = -1.

Key Concept

Factor and Remainder Theorems
Estimated Time:1m 30s
Question 7770Question

An electric scooter starts from rest and accelerates uniformly at a rate of 3 m/s23\text{ m/s}^2 for a time of 6 s6\text{ s}. What is the total distance, in meters, traveled by the scooter during this period?

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Answer: 54

Answer

The total distance traveled by the scooter is 54 m54\text{ m}.
Using the second equation of linear motion s=ut+12at2s = ut + \frac{1}{2}at^2 with u=0 m/su = 0\text{ m/s}, a=3 m/s2a = 3\text{ m/s}^2, and t=6 st = 6\text{ s} yields s=0+12(3)(36)=54 ms = 0 + \frac{1}{2}(3)(36) = 54\text{ m}.

Step-by-Step Solution

1
Identify known variables from the stem
Initial velocity u=0 m/su = 0\text{ m/s}, acceleration a=3 m/s2a = 3\text{ m/s}^2, time interval t=6 st = 6\text{ s}
Extracting given values provides the foundation for selecting the correct kinematic equation.
2
Select the appropriate equation of linear motion
s=ut+12at2s = ut + \frac{1}{2}at^2
This formula directly relates displacement ss to initial velocity uu, constant acceleration aa, and time tt.
3
Calculate the numerical displacement
s=(0 m/s)(6 s)+12(3 m/s2)(6 s)2=0+12(3)(36)=54 ms = (0\text{ m/s})(6\text{ s}) + \frac{1}{2}(3\text{ m/s}^2)(6\text{ s})^2 = 0 + \frac{1}{2}(3)(36) = 54\text{ m}
Evaluating the mathematical expression yields the final total distance.

Key Concept

Uniform Linear Acceleration
Question 7771Question

Two point charges, q1=+2.0×106 Cq_1 = +2.0 \times 10^{-6}\text{ C} and q2=2.0×106 Cq_2 = -2.0 \times 10^{-6}\text{ C}, are fixed in a vacuum separated by a distance of 0.20 m0.20\text{ m}. What is the magnitude of the net electric field intensity at the midpoint along the line joining the two charges? (Take Coulomb's constant k=9.0×109 N m2 C2k = 9.0 \times 10^9\text{ N m}^2\text{ C}^{-2})

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Answer: 3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}

Answer

3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}
The correct answer is 3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}. At the midpoint (r=0.10 mr = 0.10\text{ m}), the electric field due to the positive charge points towards the negative charge, and the field due to the negative charge also points towards the negative charge. Summing both equal field magnitudes of 1.8×106 N C11.8 \times 10^6\text{ N C}^{-1} yields 3.6×106 N C13.6 \times 10^6\text{ N C}^{-1}.

Step-by-Step Solution

1
Determine the distance from each point charge to the midpoint.
The distance r=0.20 m2=0.10 mr = \frac{0.20\text{ m}}{2} = 0.10\text{ m}.
The midpoint divides the total separation distance equally.
2
Calculate the magnitude of the electric field intensity E1E_1 created by the positive charge q1q_1 at the midpoint.
E1=kq1r2=9.0×109×2.0×106(0.10)2=1.8×106 N C1E_1 = \frac{k |q_1|}{r^2} = \frac{9.0 \times 10^9 \times 2.0 \times 10^{-6}}{(0.10)^2} = 1.8 \times 10^6\text{ N C}^{-1} directed away from q1q_1 (towards q2q_2).
Electric field vectors point away from positive charges.
3
Calculate the magnitude of the electric field intensity E2E_2 created by the negative charge q2q_2 at the midpoint.
E2=kq2r2=9.0×109×2.0×106(0.10)2=1.8×106 N C1E_2 = \frac{k |q_2|}{r^2} = \frac{9.0 \times 10^9 \times 2.0 \times 10^{-6}}{(0.10)^2} = 1.8 \times 10^6\text{ N C}^{-1} directed towards q2q_2.
Electric field vectors point towards negative charges.
4
Combine the electric field vectors vectorially to find the net field intensity.
Enet=E1+E2=1.8×106+1.8×106=3.6×106 N C1E_{\text{net}} = E_1 + E_2 = 1.8 \times 10^6 + 1.8 \times 10^6 = 3.6 \times 10^6\text{ N C}^{-1}.
Because both E1E_1 and E2E_2 point in the exact same direction (towards q2q_2), their magnitudes add directly.

Key Concept

Superposition Principle of Electric Fields
Question 7772Question

In an electric circuit, two capacitors C1=12 μFC_1 = 12\text{ }\mu\text{F} and C2=6 μFC_2 = 6\text{ }\mu\text{F} are connected in series. This series combination is then connected in parallel with a third capacitor C3C_3 of unknown value. When a direct-current potential difference of 100 V100\text{ V} is applied across the entire network, the total electrostatic energy stored in the circuit is 100 mJ100\text{ mJ}. What is the capacitance of C3C_3 in microfarads (μF\mu\text{F})?

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Answer: 16

Answer

The capacitance of C3C_3 is 16 μF16\text{ }\mu\text{F}.
First, the series combination of 12 μF12\text{ }\mu\text{F} and 6 μF6\text{ }\mu\text{F} yields an equivalent branch capacitance of 4 μF4\text{ }\mu\text{F}. Second, using E=12CeqV2E = \frac{1}{2} C_{eq} V^2 with E=0.100 JE = 0.100\text{ J} and V=100 VV = 100\text{ V} gives a total circuit equivalent capacitance of 20 μF20\text{ }\mu\text{F}. Finally, subtracting the branch capacitance from the total parallel equivalent capacitance gives C3=20 μF4 μF=16 μFC_3 = 20\text{ }\mu\text{F} - 4\text{ }\mu\text{F} = 16\text{ }\mu\text{F}.

Step-by-Step Solution

1
Calculate the effective capacitance of the series branch containing C1C_1 and C2C_2
C12=4 μFC_{12} = 4\text{ }\mu\text{F}
Capacitors in series combine reciprocally: 1C12=1C1+1C2=112+16=312    C12=4 μF\frac{1}{C_{12}} = \frac{1}{C_1} + \frac{1}{C_2} = \frac{1}{12} + \frac{1}{6} = \frac{3}{12} \implies C_{12} = 4\text{ }\mu\text{F}.
2
Determine the total equivalent capacitance CeqC_{eq} of the circuit using the given stored energy and voltage
Ceq=20 μFC_{eq} = 20\text{ }\mu\text{F}
Energy stored in a capacitor network is E=12CeqV2E = \frac{1}{2} C_{eq} V^2. Rearranging gives Ceq=2EV2=2×0.100 J(100 V)2=20×106 F=20 μFC_{eq} = \frac{2E}{V^2} = \frac{2 \times 0.100\text{ J}}{(100\text{ V})^2} = 20 \times 10^{-6}\text{ F} = 20\text{ }\mu\text{F}.
3
Calculate the unknown capacitance C3C_3 from the parallel combination formula
C3=16 μFC_3 = 16\text{ }\mu\text{F}
Because the branch C12C_{12} and C3C_3 are in parallel, Ceq=C12+C3    20 μF=4 μF+C3    C3=16 μFC_{eq} = C_{12} + C_3 \implies 20\text{ }\mu\text{F} = 4\text{ }\mu\text{F} + C_3 \implies C_3 = 16\text{ }\mu\text{F}.

Key Concept

Series and parallel combinations of capacitors combined with electrostatic energy storage
Estimated Time:2m 0s
Question 7773Question

A water wave with a frequency of 20 Hz20\text{ Hz} and a wavelength of 0.60 m0.60\text{ m} in deep water enters a shallow region where its speed becomes 8.0 m s18.0\text{ m s}^{-1}. What is the wavelength of the wave in the shallow region?

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Answer: 0.40 m0.40\text{ m}

Answer

The wavelength of the wave in the shallow region is 0.40 m0.40\text{ m}.
When a wave passes from one medium into another, its frequency remains constant because frequency depends only on the source. Applying the wave equation v=fλv = f\lambda to the shallow region gives λ=vf=8.0 m s120 Hz=0.40 m\lambda = \frac{v}{f} = \frac{8.0\text{ m s}^{-1}}{20\text{ Hz}} = 0.40\text{ m}.

Step-by-Step Solution

1
Identify the constant parameter during wave refraction.
The frequency of the wave remains f=20 Hzf = 20\text{ Hz}.
Frequency is determined entirely by the source producing the wave and does not change upon entering a new medium.
2
Calculate the new wavelength using the wave equation v=fλv = f\lambda.
\(\lambda = \frac{v}{f} = \frac{8.0\text{ m s}^{-1}}{20\text{ Hz}} = 0.40\text{ m}\).
Dividing the wave speed in the new medium by the constant frequency yields the wavelength in that medium.

Key Concept

Constancy of wave frequency during refraction across media boundaries
Question 7774Question

Match each physical quantity listed on the left with its corresponding SI unit expressed strictly in terms of fundamental (base) units on the right.

Click a left item, then click its matching right item

Items

Electric permittivity of free space (ε0\varepsilon_0)
Magnetic permeability of free space (μ0\mu_0)
Thermal conductivity (kk)
Specific heat capacity (cc)

Matches

Show answer & explanation

Answer

Electric permittivity of free space maps to kg1m3s4A2\text{kg}^{-1}\cdot\text{m}^{-3}\cdot\text{s}^4\cdot\text{A}^2, Magnetic permeability of free space maps to kgms2A2\text{kg}\cdot\text{m}\cdot\text{s}^{-2}\cdot\text{A}^{-2}, Thermal conductivity maps to kgms3K1\text{kg}\cdot\text{m}\cdot\text{s}^{-3}\cdot\text{K}^{-1}, and Specific heat capacity maps to m2s2K1\text{m}^2\cdot\text{s}^{-2}\cdot\text{K}^{-1}.
Each physical quantity is matched to its exact fundamental unit expression obtained by substituting basic formulas into SI base units (kg\text{kg}, m\text{m}, s\text{s}, A\text{A}, K\text{K}). Electric permittivity resolves to kg1m3s4A2\text{kg}^{-1}\cdot\text{m}^{-3}\cdot\text{s}^4\cdot\text{A}^2, magnetic permeability resolves to kgms2A2\text{kg}\cdot\text{m}\cdot\text{s}^{-2}\cdot\text{A}^{-2}, thermal conductivity resolves to kgms3K1\text{kg}\cdot\text{m}\cdot\text{s}^{-3}\cdot\text{K}^{-1}, and specific heat capacity resolves to m2s2K1\text{m}^2\cdot\text{s}^{-2}\cdot\text{K}^{-1}.

Step-by-Step Solution

1
Derive the base SI units for Electric permittivity of free space (ε0\varepsilon_0).
From Coulomb's Law, F=q1q24πε0r2    ε0=q1q24πFr2F = \frac{q_1 q_2}{4\pi \varepsilon_0 r^2} \implies \varepsilon_0 = \frac{q_1 q_2}{4\pi F r^2}. Expressing terms in SI fundamental units: charge q=Asq = \text{A}\cdot\text{s}, force F=kgms2F = \text{kg}\cdot\text{m}\cdot\text{s}^{-2}, distance r=mr = \text{m}. Thus, [ε0]=(As)2(kgms2)m2=kg1m3s4A2[\varepsilon_0] = \frac{(\text{A}\cdot\text{s})^2}{(\text{kg}\cdot\text{m}\cdot\text{s}^{-2})\cdot\text{m}^2} = \text{kg}^{-1}\cdot\text{m}^{-3}\cdot\text{s}^4\cdot\text{A}^2.
Relating derived electromagnetic quantities to fundamental SI units via governing physical equations.
2
Derive the base SI units for Magnetic permeability of free space (μ0\mu_0).
From the force per unit length between parallel current-carrying conductors, FL=μ0I1I22πr    μ0=2πFrI1I2L\frac{F}{L} = \frac{\mu_0 I_1 I_2}{2\pi r} \implies \mu_0 = \frac{2\pi F r}{I_1 I_2 L}. Units: [μ0]=(kgms2)mA2m=kgms2A2[\mu_0] = \frac{(\text{kg}\cdot\text{m}\cdot\text{s}^{-2})\cdot\text{m}}{\text{A}^2\cdot\text{m}} = \text{kg}\cdot\text{m}\cdot\text{s}^{-2}\cdot\text{A}^{-2}.
Using Ampère's force law to solve for magnetic permeability in base units.
3
Derive the base SI units for Thermal conductivity (kk).
From Fourier's Law of Heat Conduction, Qt=kAΔTΔx    k=QΔxtAΔT\frac{Q}{t} = k A \frac{\Delta T}{\Delta x} \implies k = \frac{Q \cdot \Delta x}{t A \Delta T}. Heat energy Q=kgm2s2Q = \text{kg}\cdot\text{m}^2\cdot\text{s}^{-2}, time t=st = \text{s}, area A=m2A = \text{m}^2, thickness Δx=m\Delta x = \text{m}, temperature difference ΔT=K\Delta T = \text{K}. Thus, [k]=(kgm2s2)msm2K=kgms3K1[k] = \frac{(\text{kg}\cdot\text{m}^2\cdot\text{s}^{-2})\cdot\text{m}}{\text{s}\cdot\text{m}^2\cdot\text{K}} = \text{kg}\cdot\text{m}\cdot\text{s}^{-3}\cdot\text{K}^{-1}.
Connecting thermal conduction equations to fundamental mechanics and thermodynamic units.
4
Derive the base SI units for Specific heat capacity (cc).
From Q=mcΔT    c=QmΔTQ = m c \Delta T \implies c = \frac{Q}{m \Delta T}. Units: [c]=kgm2s2kgK=m2s2K1[c] = \frac{\text{kg}\cdot\text{m}^2\cdot\text{s}^{-2}}{\text{kg}\cdot\text{K}} = \text{m}^2\cdot\text{s}^{-2}\cdot\text{K}^{-1}.
Applying the defining equation of heat capacity to reduce the unit to fundamental base units.

Key Concept

Derivation of complex derived SI units from fundamental base units using fundamental physical laws.
Question 7775Question

A trader deposited 40,000\text{₦}40,000 in a microfinance bank offering compound interest at the rate of 10%10\% per annum, compounded annually. What is the total interest earned by the trader at the end of 22 years?

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Answer: 8,400\text{₦}8,400

Answer

The total interest earned by the trader at the end of 22 years is 8,400\text{₦}8,400.
Using the compound interest formula A=P(1+r)nA = P(1 + r)^n, the total accumulated amount after 2 years is 40,000×(1.1)2=48,40040,000 \times (1.1)^2 = \text{₦}48,400. Subtracting the original principal of 40,000\text{₦}40,000 gives the compound interest earned: 48,40040,000=8,40048,400 - 40,000 = \text{₦}8,400.

Step-by-Step Solution

1
Calculate the total accumulated amount (AA) using the compound interest formula A=P(1+R100)nA = P\left(1 + \frac{R}{100}\right)^n.
A=40,000(1+10100)2=40,000×(1.1)2=40,000×1.21=48,400A = 40,000\left(1 + \frac{10}{100}\right)^2 = 40,000 \times (1.1)^2 = 40,000 \times 1.21 = \text{₦}48,400.
The compound interest formula yields the total value of the investment after 2 years.
2
Subtract the initial principal (PP) from the total accumulated amount (AA) to find the compound interest (II).
I=AP=48,40040,000=8,400I = A - P = 48,400 - 40,000 = \text{₦}8,400.
Interest earned is the difference between total final amount and initial principal.

Key Concept

Calculation of compound interest vs total accumulated amount
Question 7776Question

Which of the following is the set of real values of xx that satisfies the inequality 3x42x+53\frac{3 - x}{4} \le \frac{2x + 5}{3}?

Show answer & explanation

Answer: x1x \ge -1

Answer

The set of real values of xx that satisfies the inequality is x1x \ge -1.
Multiplying through by 12 gives 93x8x+209 - 3x \le 8x + 20. Grouping terms results in 11x11-11x \le 11. Dividing by 11-11 requires reversing the inequality sign from \le to \ge, giving the solution x1x \ge -1.

Step-by-Step Solution

1
Clear the denominators by multiplying both sides of the inequality by the lowest common multiple, 12.
3(3x)4(2x+5)3(3 - x) \le 4(2x + 5)
Eliminating fractions simplifies the algebraic expression.
2
Expand both sides by distributing the multipliers.
93x8x+209 - 3x \le 8x + 20
Prepares terms for grouping variables on one side and constants on the other.
3
Collect all terms containing xx on the left side and constant terms on the right side.
3x8x209    11x11-3x - 8x \le 20 - 9 \implies -11x \le 11
Isolates the linear variable term.
4
Divide both sides by 11-11 and flip the inequality sign.
x1x \ge -1
Dividing or multiplying an inequality by a negative number reverses the direction of the inequality sign.

Key Concept

Linear Inequalities and Reversing Inequality Sign on Division by Negative Numbers
Question 7777Question

A student obtained a mean score of 6262 in 55 subjects. After the score of a 6th6\text{th} subject was added, the overall mean score became 6565. What is the score obtained in the 6th6\text{th} subject?

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Answer: 80

Answer

The score obtained in the 6th subject is 80.
The sum of scores for the first 5 subjects is 5×62=3105 \times 62 = 310. With the 6th subject included, the total sum of scores becomes 6×65=3906 \times 65 = 390. The score of the 6th subject is the difference between these two totals: 390310=80390 - 310 = 80.

Step-by-Step Solution

1
Calculate the total score of the initial 5 subjects
310
The sum of scores for ungrouped data is equal to the number of data items multiplied by the mean: 5 × 62 = 310.
2
Calculate the total score of all 6 subjects after including the new score
390
The new total score is obtained by multiplying the new count of subjects by the new mean: 6 × 65 = 390.
3
Determine the score of the 6th subject
80
The difference between the total score of 6 subjects and the total score of 5 subjects gives the score of the 6th subject: 390 - 310 = 80.

Key Concept

Calculating a missing data value given the mean of ungrouped data before and after addition
Question 7778Question

A brass container with an initial capacity of 500 cm3500\text{ cm}^3 at 20C20^\circ\text{C} is filled completely with ethanol. When the container and its contents are uniformly heated to 70C70^\circ\text{C}, a volume of 12 cm312\text{ cm}^3 of ethanol overflows from the container. Given that the linear expansivity of brass is 2.0×105 K12.0 \times 10^{-5}\text{ K}^{-1}, calculate the real cubic expansivity of ethanol in units of 104 K110^{-4}\text{ K}^{-1}.

Show answer & explanation

Answer: 5.4

Answer

The real cubic expansivity of ethanol is 5.4×104 K15.4 \times 10^{-4}\text{ K}^{-1}, which corresponds to a value of 5.45.4 in units of 104 K110^{-4}\text{ K}^{-1}.
The real volume increase of a liquid consists of the apparent expansion (observed overflow volume) plus the volume expansion of the container itself. By finding the apparent cubic expansivity γa=12500×50=4.8×104 K1\gamma_a = \frac{12}{500 \times 50} = 4.8 \times 10^{-4}\text{ K}^{-1} and adding the vessel's cubic expansivity γv=3×2.0×105=0.6×104 K1\gamma_v = 3 \times 2.0 \times 10^{-5} = 0.6 \times 10^{-4}\text{ K}^{-1}, we obtain the real cubic expansivity γr=5.4×104 K1\gamma_r = 5.4 \times 10^{-4}\text{ K}^{-1}, which yields 5.45.4 in the required units.

Step-by-Step Solution

1
Determine the temperature increase of the system
\Delta T = 70^\circ\text{C} - 20^\circ\text{C} = 50\text{ K}
The thermal expansion is driven by the change in temperature.
2
Calculate the apparent cubic expansivity of ethanol (\gamma_a)
\gamma_a = \frac{\Delta V_{overflow}}{V_0 \cdot \Delta T} = \frac{12\text{ cm}^3}{500\text{ cm}^3 \times 50\text{ K}} = 4.8 \times 10^{-4}\text{ K}^{-1}
The overflow volume represents the apparent volume increase of the liquid relative to the expanding vessel.
3
Calculate the cubic expansivity of the brass vessel (\gamma_v)
\gamma_v = 3 \times \alpha_{brass} = 3 \times 2.0 \times 10^{-5}\text{ K}^{-1} = 6.0 \times 10^{-5}\text{ K}^{-1} = 0.6 \times 10^{-4}\text{ K}^{-1}
Cubic expansivity of a solid vessel is three times its linear expansivity.
4
Compute the real cubic expansivity of ethanol (\gamma_r)
\gamma_r = \gamma_a + \gamma_v = 4.8 \times 10^{-4}\text{ K}^{-1} + 0.6 \times 10^{-4}\text{ K}^{-1} = 5.4 \times 10^{-4}\text{ K}^{-1}
The real expansion of a liquid is the sum of its apparent expansion and the expansion of the containing vessel.

Key Concept

Relationship between Real and Apparent Cubic Expansivity of Liquids
Question 7779Question

A neutral insulated conductor loses 5.0×10135.0 \times 10^{13} electrons during an electrostatics experiment. What is the magnitude of the net electric charge, in microcoulombs (μC\mu\text{C}), acquired by the conductor? (Take elementary charge e=1.6×1019 Ce = 1.6 \times 10^{-19}\text{ C})

Show answer & explanation

Answer: 8

Answer

The magnitude of the net electric charge acquired by the conductor is 8 μC8\text{ }\mu\text{C}.
According to the principle of charge quantization, the total electric charge QQ is calculated using Q=neQ = n e. Multiplying 5.0×10135.0 \times 10^{13} electrons by 1.6×1019 C1.6 \times 10^{-19}\text{ C} yields 8.0×106 C8.0 \times 10^{-6}\text{ C}, which converts to 8 μC8\text{ }\mu\text{C}.

Step-by-Step Solution

1
Identify the relevant formula for quantization of charge.
The net charge acquired is given by Q=neQ = n e.
Electric charge is quantized, so the total charge magnitude equals the number of transferred electrons multiplied by the magnitude of charge on a single electron.
2
Calculate the magnitude of charge in Coulombs.
Q=(5.0×1013)×(1.6×1019 C)=8.0×106 CQ = (5.0 \times 10^{13}) \times (1.6 \times 10^{-19}\text{ C}) = 8.0 \times 10^{-6}\text{ C}.
Multiplying the quantity of removed electrons by the elementary charge gives total charge in Coulombs.
3
Convert the calculated value from Coulombs to microcoulombs.
8.0×106 C=8 μC8.0 \times 10^{-6}\text{ C} = 8\text{ }\mu\text{C}.
Since 1 μC=106 C1\text{ }\mu\text{C} = 10^{-6}\text{ C}, dividing 8.0×1068.0 \times 10^{-6} by 10610^{-6} yields 8.

Key Concept

Quantization of Electric Charge
Question 7780Question

During a head-on collision in Rutherford's α\alpha-particle scattering experiment, an α\alpha-particle of initial speed vv approaches a stationary heavy nucleus. The distance of closest approach achieved by the α\alpha-particle is r0r_0. If the initial speed of the α\alpha-particle is increased to 2v2v, what will be the new distance of closest approach in terms of r0r_0?

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Answer: r04\frac{r_0}{4}

Answer

The new distance of closest approach will be r04\frac{r_0}{4}.
At the distance of closest approach, the entire initial kinetic energy of the α\alpha-particle is converted into electric potential energy: Ek=12mv2=keq1q2rE_k = \frac{1}{2}mv^2 = \frac{k_e q_1 q_2}{r}. Rearranging for rr gives r=2keq1q2mv2r = \frac{2k_e q_1 q_2}{m v^2}, showing that rr is inversely proportional to v2v^2. When the initial speed is doubled to 2v2v, the kinetic energy increases by a factor of 22=42^2 = 4. Consequently, the distance of closest approach is reduced to one-fourth of its initial value, r04\frac{r_0}{4}.

Step-by-Step Solution

1
Apply conservation of mechanical energy at the distance of closest approach.
Initial kinetic energy equals electrostatic potential energy at distance r0r_0: 12mv2=14πε0q1q2r0\frac{1}{2} m v^2 = \frac{1}{4\pi\varepsilon_0} \frac{q_1 q_2}{r_0}.
At the distance of closest approach, the α\alpha-particle momentarily stops, converting all kinetic energy into electric potential energy.
2
Express the distance of closest approach r0r_0 in terms of initial speed vv.
r0=2q1q24πε0mv21v2r_0 = \frac{2 q_1 q_2}{4\pi\varepsilon_0 m v^2} \propto \frac{1}{v^2}.
Rearranging the energy conservation equation demonstrates that distance of closest approach is inversely proportional to v2v^2.
3
Substitute the new speed v=2vv' = 2v into the proportion.
r1(2v)2=14v2=r04r' \propto \frac{1}{(2v)^2} = \frac{1}{4v^2} = \frac{r_0}{4}.
Doubling the speed quadruples the kinetic energy, reducing the distance required to bring the particle to rest by a factor of 4.

Key Concept

Distance of Closest Approach in Rutherford Scattering
Estimated Time:2m 0s
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