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Question 901Question

A cylindrical metal rivet has a diameter of 2.50 cm2.50\text{ cm} at a room temperature of 25C25^\circ\text{C}. It needs to be inserted into a hole of diameter 2.49 cm2.49\text{ cm} in a structural frame. By how many kelvins must the rivet be cooled so that its diameter shrinks to just match the diameter of the hole? (Linear expansivity of the metal is 2.0×105 K12.0 \times 10^{-5}\text{ K}^{-1}).

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Answer: 200

Answer

The rivet must be cooled by 200 K.
Thermal expansion or contraction of a linear dimension (such as diameter) is governed by Δd=d0αΔT\Delta d = d_0 \alpha \Delta T. Substituting Δd=0.01 cm\Delta d = -0.01\text{ cm}, d0=2.50 cmd_0 = 2.50\text{ cm}, and α=2.0×105 K1\alpha = 2.0 \times 10^{-5}\text{ K}^{-1} gives 0.01=2.50×(2.0×105)×ΔT-0.01 = 2.50 \times (2.0 \times 10^{-5}) \times \Delta T, leading to ΔT=200 K\Delta T = -200\text{ K}. Hence, cooling by 200 K is required.

Step-by-Step Solution

1
Calculate the required change in diameter
\Delta d = 2.49\text{ cm} - 2.50\text{ cm} = -0.01\text{ cm}
The diameter of the rivet must decrease from 2.50 cm to 2.49 cm to fit into the hole.
2
Set up the linear expansion equation
\Delta d = d_0 \alpha \Delta T
Linear contraction/expansion applies directly to any linear dimension of a solid, including diameter.
3
Substitute given values into the equation
-0.01\text{ cm} = (2.50\text{ cm}) \times (2.0 \times 10^{-5}\text{ K}^{-1}) \times \Delta T
Substitute initial diameter, linear expansivity, and change in diameter.
4
Solve for the temperature change
\Delta T = \frac{-0.01}{5.0 \times 10^{-5}} = -200\text{ K}
Dividing the change in length by the product of initial length and linear expansivity yields the temperature change.

Key Concept

Thermal Contraction and Linear Expansivity of Solids
Question 902Question

In an electrical power station, two independent backup transformers, T1T_1 and T2T_2, operate simultaneously during power surges. The probability that T1T_1 fails during a surge is 0.150.15, and the probability that T2T_2 fails during the same surge is 0.200.20. What is the probability that at least one transformer functions correctly during a power surge?

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Answer: 0.97

Answer

0.97
The failure probabilities are P(F1)=0.15P(F_1) = 0.15 and P(F2)=0.20P(F_2) = 0.20. By the multiplication law for independent events, the probability of both failing is P(F1F2)=0.15×0.20=0.03P(F_1 \cap F_2) = 0.15 \times 0.20 = 0.03. Using the complement rule, the probability of at least one functioning correctly is 1P(F1F2)=10.03=0.971 - P(F_1 \cap F_2) = 1 - 0.03 = 0.97.

Step-by-Step Solution

1
Determine the joint probability of both transformers failing.
P(F1F2)=0.15×0.20=0.03P(F_1 \cap F_2) = 0.15 \times 0.20 = 0.03
Since the operational failures of the two transformers are independent events, the probability of both failing together is the product of their individual failure probabilities.
2
Calculate the probability that at least one transformer functions correctly.
P(at least one functions)=10.03=0.97P(\text{at least one functions}) = 1 - 0.03 = 0.97
The event that at least one transformer functions is the complement of the event that both transformers fail simultaneously.

Key Concept

Independent Compound Events and the Complement Rule
Question 903Question

A projectile is launched from level ground with an initial speed of 25 m/s25\text{ m/s} at an angle θ\theta to the horizontal such that sinθ=0.80\sin\theta = 0.80. Calculate the maximum height reached by the projectile in meters. [Take g=10 m/s2g = 10\text{ m/s}^2]

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Answer: 20

Answer

The maximum height reached by the projectile is 20 m20\text{ m}.
The vertical component of the initial launch velocity is uy=usinθ=25×0.80=20 m/su_y = u \sin\theta = 25 \times 0.80 = 20\text{ m/s}. Using the equation for maximum height H=uy22gH = \frac{u_y^2}{2g}, we substitute uy=20 m/su_y = 20\text{ m/s} and g=10 m/s2g = 10\text{ m/s}^2 to obtain H=40020=20 mH = \frac{400}{20} = 20\text{ m}.

Step-by-Step Solution

1
Calculate the initial vertical velocity component (uyu_y)
uy=25 m/s×0.80=20 m/su_y = 25\text{ m/s} \times 0.80 = 20\text{ m/s}
Only the vertical component of velocity determines the maximum height reached.
2
Calculate the maximum height (HH) using kinematic equations
H=uy22g=2022×10=20 mH = \frac{u_y^2}{2g} = \frac{20^2}{2 \times 10} = 20\text{ m}
At maximum height, the vertical component of velocity becomes zero.

Key Concept

Maximum height of a projectile depends entirely on its initial vertical component of velocity and acceleration due to gravity.
Question 904Question

A cylindrical brass sleeve has an internal diameter of 5.000 cm5.000\text{ cm} at a room temperature of 20C20^\circ\text{C}. It is to be shrink-fitted onto a solid shaft of diameter 5.012 cm5.012\text{ cm} (also at 20C20^\circ\text{C}). Assuming the linear expansivity of brass is 2.0×105 K12.0 \times 10^{-5}\text{ K}^{-1}, what is the minimum temperature, in C^\circ\text{C}, to which the brass sleeve must be heated so that it just slips over the shaft?

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Answer: 140

Answer

140 °C
The required expansion in internal diameter is Δd=5.012 cm5.000 cm=0.012 cm\Delta d = 5.012\text{ cm} - 5.000\text{ cm} = 0.012\text{ cm}. Using the linear expansion relation Δd=d0αΔT\Delta d = d_0 \alpha \Delta T, the required temperature change is ΔT=0.0125.000×2.0×105=120C\Delta T = \frac{0.012}{5.000 \times 2.0 \times 10^{-5}} = 120^\circ\text{C}. Adding this to the initial temperature of 20C20^\circ\text{C} gives a final minimum temperature of 140C140^\circ\text{C}.

Step-by-Step Solution

1
Determine the required increase in internal diameter (Δd\Delta d) of the brass sleeve
Δd=5.012 cm5.000 cm=0.012 cm\Delta d = 5.012\text{ cm} - 5.000\text{ cm} = 0.012\text{ cm}
The sleeve's internal diameter must expand until it equals the shaft diameter.
2
Apply the linear expansion formula Δd=d0αΔT\Delta d = d_0 \alpha \Delta T to find the temperature rise ΔT\Delta T
ΔT=0.012 cm5.000 cm×2.0×105 K1=0.0121.0×104=120 K\Delta T = \frac{0.012\text{ cm}}{5.000\text{ cm} \times 2.0 \times 10^{-5}\text{ K}^{-1}} = \frac{0.012}{1.0 \times 10^{-4}} = 120\text{ K}
Linear dimensions such as diameter expand in direct proportion to the linear expansivity coefficient α\alpha.
3
Calculate the final temperature T2T_2
T2=T1+ΔT=20C+120C=140CT_2 = T_1 + \Delta T = 20^\circ\text{C} + 120^\circ\text{C} = 140^\circ\text{C}
The final temperature is found by adding the temperature increase to the initial temperature.

Key Concept

Linear Expansivity and One-Dimensional Expansion of Curved Boundaries
Question 905Question

Given the function f(x)=5x24x+3f(x) = 5x^2 - 4x + 3, what is the numerical value of its derivative at x=2x = 2 when evaluated using the first principles limit definition limh0f(x+h)f(x)h\lim_{h \to 0} \frac{f(x+h) - f(x)}{h}?

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Answer: 16

Answer

The numerical value of the derivative of f(x)=5x24x+3f(x) = 5x^2 - 4x + 3 at x=2x = 2 is 16.
Evaluating the first principles definition limh0f(x+h)f(x)h\lim_{h \to 0} \frac{f(x+h) - f(x)}{h} for f(x)=5x24x+3f(x) = 5x^2 - 4x + 3 yields the derivative f(x)=10x4f'(x) = 10x - 4. Substituting x=2x = 2 yields 10(2)4=1610(2) - 4 = 16.

Step-by-Step Solution

1
Determine the expanded form of f(x+h)f(x+h)
f(x+h)=5(x+h)24(x+h)+3=5x2+10xh+5h24x4h+3f(x+h) = 5(x+h)^2 - 4(x+h) + 3 = 5x^2 + 10xh + 5h^2 - 4x - 4h + 3
Evaluating the function at x+hx+h requires expanding the square and distributing the constant factors.
2
Compute the difference f(x+h)f(x)f(x+h) - f(x)
f(x+h)f(x)=(5x2+10xh+5h24x4h+3)(5x24x+3)=10xh+5h24hf(x+h) - f(x) = (5x^2 + 10xh + 5h^2 - 4x - 4h + 3) - (5x^2 - 4x + 3) = 10xh + 5h^2 - 4h
Subtracting f(x)f(x) cancels terms independent of hh.
3
Form and simplify the difference quotient f(x+h)f(x)h\frac{f(x+h) - f(x)}{h}
10xh+5h24hh=10x+5h4\frac{10xh + 5h^2 - 4h}{h} = 10x + 5h - 4
Factoring hh out of the numerator allows division by hh for non-zero hh.
4
Evaluate the limit as h0h \to 0
f(x)=limh0(10x+5h4)=10x4f'(x) = \lim_{h \to 0} (10x + 5h - 4) = 10x - 4
Taking the limit produces the general derivative function dydx\frac{\mathrm{d}y}{\mathrm{d}x}.
5
Substitute x=2x = 2 into the derivative
f(2)=10(2)4=16f'(2) = 10(2) - 4 = 16
Evaluating at x=2x = 2 gives the instantaneous rate of change at that point.

Key Concept

Differentiation from First Principles
Estimated Time:1m 30s
Question 906Question

Given that (kx3+12cos(3x))dx=4x4+4sin(3x)+C\int \left( k x^3 + 12\cos(3x) \right) dx = 4x^4 + 4\sin(3x) + C, where CC is the arbitrary constant of integration, what is the numerical value of the constant kk?

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Answer: 16

Answer

The numerical value of the constant kk is 16.
Integrating kx3+12cos(3x)kx^3 + 12\cos(3x) with respect to xx yields k4x4+4sin(3x)+C\frac{k}{4}x^4 + 4\sin(3x) + C. Comparing the coefficient of x4x^4 with the given result 4x4+4sin(3x)+C4x^4 + 4\sin(3x) + C gives k4=4\frac{k}{4} = 4, which leads to k=16k = 16.

Step-by-Step Solution

1
Integrate the polynomial and trigonometric terms separately using standard integration rules.
\int (kx^3 + 12\cos(3x)) dx = \frac{k}{4}x^4 + 4\sin(3x) + C
Applying the power rule xndx=xn+1n+1\int x^n dx = \frac{x^{n+1}}{n+1} gives kx3dx=k4x4\int kx^3 dx = \frac{k}{4}x^4, and applying cos(ax)dx=sin(ax)a\int \cos(ax) dx = \frac{\sin(ax)}{a} gives 12cos(3x)dx=123sin(3x)=4sin(3x)\int 12\cos(3x) dx = \frac{12}{3}\sin(3x) = 4\sin(3x).
2
Equate the integrated expression to the right-hand side of the given equation.
\frac{k}{4}x^4 + 4\sin(3x) + C = 4x^4 + 4\sin(3x) + C
Both sides represent the same antiderivative of the function.
3
Equate corresponding coefficients of x4x^4 to solve for kk.
k = 16
\frac{k}{4} = 4 \implies k = 4 \times 4 = 16.

Key Concept

Indefinite Integration of Polynomial and Trigonometric Functions
Question 907Question

The 5th5^{\text{th}} term of an arithmetic progression (AP) is 1818 and its 11th11^{\text{th}} term is 4242. Calculate the value of the 20th20^{\text{th}} term of this progression.

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Answer: 78

Answer

78
Using the AP general term formula Tn=a+(n1)dT_n = a + (n-1)d, the equations a+4d=18a + 4d = 18 and a+10d=42a + 10d = 42 yield d=4d = 4 and a=2a = 2. Evaluating T20=2+19(4)T_{20} = 2 + 19(4) yields 7878.

Step-by-Step Solution

1
Set up simultaneous equations using the general term formula Tn=a+(n1)dT_n = a + (n-1)d
a+4d=18a + 4d = 18 and a+10d=42a + 10d = 42
Relate given terms to the first term aa and common difference dd.
2
Solve for the common difference dd
6d=24    d=46d = 24 \implies d = 4
Subtracting the 5th term equation from the 11th term equation eliminates aa.
3
Solve for the first term aa
a+16=18    a=2a + 16 = 18 \implies a = 2
Substitute the value of dd back into the first equation.
4
Calculate the 20th term
T20=2+19(4)=78T_{20} = 2 + 19(4) = 78
Apply the nth term formula for n=20n = 20.

Key Concept

Determining terms of an Arithmetic Progression using simultaneous equations
Estimated Time:1m 30s
Question 908Question

A potentiometer wire of length 100 cm100\text{ cm} has a resistance of 10 Ω10\text{ }\Omega. It is connected in series with a driver cell of electromotive force 3.0 V3.0\text{ V} and internal resistance 2.0 Ω2.0\text{ }\Omega, alongside an external series resistor of 8.0 Ω8.0\text{ }\Omega. A test cell of unknown electromotive force EE gives a balance point at a length of 60 cm60\text{ cm} from the zero end of the wire. What is the value of EE in volts?

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Answer: 0.9

Answer

The electromotive force of the test cell is 0.9 V0.9\text{ V}.
The e.m.f. of the test cell is balanced by the potential difference across a length of 60 cm60\text{ cm} of the potentiometer wire. Accounting for the driver cell's internal resistance (2.0 Ω2.0\text{ }\Omega), external series resistor (8.0 Ω8.0\text{ }\Omega), and wire resistance (10 Ω10\text{ }\Omega), the total resistance of the primary circuit is 20.0 Ω20.0\text{ }\Omega. This yields a primary current of 0.15 A0.15\text{ A} and a potential drop across the wire of 1.5 V1.5\text{ V}. The resulting potential gradient is 0.015 V/cm0.015\text{ V/cm}, which when multiplied by the balance length of 60 cm60\text{ cm} gives an e.m.f. of 0.9 V0.9\text{ V}.

Step-by-Step Solution

1
Calculate total resistance in the primary driver circuit
Rtotal=10 Ω+2.0 Ω+8.0 Ω=20.0 ΩR_{total} = 10\text{ }\Omega + 2.0\text{ }\Omega + 8.0\text{ }\Omega = 20.0\text{ }\Omega
The driver cell's internal resistance, potentiometer wire, and external series resistor are connected in series.
2
Calculate the current flowing through the potentiometer wire
I=3.0 V20.0 Ω=0.15 AI = \frac{3.0\text{ V}}{20.0\text{ }\Omega} = 0.15\text{ A}
Apply Ohm's law to the complete primary circuit.
3
Find the voltage drop across the potentiometer wire
Vwire=0.15 A×10 Ω=1.5 VV_{wire} = 0.15\text{ A} \times 10\text{ }\Omega = 1.5\text{ V}
The potential difference across the wire depends on its resistance and the primary current.
4
Determine the potential gradient along the wire
k=1.5 V100 cm=0.015 V/cmk = \frac{1.5\text{ V}}{100\text{ cm}} = 0.015\text{ V/cm}
Potential gradient is the potential drop per unit length of the wire.
5
Calculate the e.m.f. of the unknown test cell
E=0.015 V/cm×60 cm=0.9 VE = 0.015\text{ V/cm} \times 60\text{ cm} = 0.9\text{ V}
At the balance point, no current flows from the test cell, so its e.m.f. equals the potential drop across the balance length.

Key Concept

Potentiometer principle and potential gradient
Estimated Time:2m 0s
Question 909Question

A right-angled triangle has a perimeter of 60 cm60\text{ cm} and a hypotenuse of length 25 cm25\text{ cm}. What is the area of the triangle in cm2\text{cm}^2?

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Answer: 150

Answer

150
Let the perpendicular sides of the right-angled triangle be aa and bb, and the hypotenuse be c=25 cmc = 25\text{ cm}. From the perimeter, a+b+25=60a + b + 25 = 60, so a+b=35 cma + b = 35\text{ cm}. By the Pythagorean theorem, a2+b2=252=625a^2 + b^2 = 25^2 = 625. Squaring both sides of a+b=35a + b = 35 yields (a+b)2=a2+b2+2ab=352=1225(a + b)^2 = a^2 + b^2 + 2ab = 35^2 = 1225. Substituting a2+b2=625a^2 + b^2 = 625 gives 625+2ab=1225    2ab=600    ab=300625 + 2ab = 1225 \implies 2ab = 600 \implies ab = 300. The area of the right-angled triangle is 12ab=12×300=150 cm2\frac{1}{2}ab = \frac{1}{2} \times 300 = 150\text{ cm}^2.

Step-by-Step Solution

1
Determine the sum of the two legs from the perimeter
a+b=35 cma + b = 35\text{ cm}
The perimeter of the triangle is a+b+c=60 cma + b + c = 60\text{ cm}, where the hypotenuse c=25 cmc = 25\text{ cm}.
2
Use the Pythagorean theorem for the sum of squares of the legs
a2+b2=625a^2 + b^2 = 625
In any right-angled triangle with hypotenuse 25 cm25\text{ cm}, a2+b2=252=625a^2 + b^2 = 25^2 = 625.
3
Expand (a+b)2(a + b)^2 to find the product of the legs abab
1225=625+2ab    2ab=600    ab=3001225 = 625 + 2ab \implies 2ab = 600 \implies ab = 300
Using the algebraic identity (a+b)2=a2+b2+2ab(a + b)^2 = a^2 + b^2 + 2ab allows determining abab directly without solving for individual side lengths.
4
Calculate the area of the right-angled triangle
\text{Area} = 150\text{ cm}^2
The area of a right-angled triangle with perpendicular sides aa and bb is given by 12ab\frac{1}{2}ab.

Key Concept

Perimeter and Area of Right-Angled Triangles using Algebraic Identities
Question 910Question

A uniform metallic conductor of length 200m200\,\text{m} and cross-sectional area 2.0×106m22.0 \times 10^{-6}\,\text{m}^2 has a resistivity of 1.6×108Ωm1.6 \times 10^{-8}\,\Omega\cdot\text{m} at an initial temperature of 20C20\,^\circ\text{C}. The temperature coefficient of resistivity for the material is 5.0×103C15.0 \times 10^{-3}\,^\circ\text{C}^{-1}. If the operating temperature of the conductor increases to 120C120\,^\circ\text{C} while it is connected across a constant potential difference of 12V12\,\text{V}, what is the magnitude of the electric current flowing through the conductor in amperes?

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Answer: 5

Answer

The electric current flowing through the conductor is 5.0A5.0\,\text{A}.
The temperature change of 100C100\,^\circ\text{C} increases the resistivity of the material from 1.6×108Ωm1.6 \times 10^{-8}\,\Omega\cdot\text{m} to 2.4×108Ωm2.4 \times 10^{-8}\,\Omega\cdot\text{m} via ρ=ρ0(1+αΔT)\rho = \rho_0(1 + \alpha \Delta T). Substituting this updated resistivity into R=ρLAR = \frac{\rho L}{A} gives a resistance of 2.4Ω2.4\,\Omega. Applying Ohm's Law I=VRI = \frac{V}{R} with a potential difference of 12V12\,\text{V} yields 5.0A5.0\,\text{A}.

Step-by-Step Solution

1
Calculate the temperature difference
ΔT=100C\Delta T = 100\,^\circ\text{C}
The temperature change relative to the reference temperature dictates the change in resistivity.
2
Calculate the resistivity at the final temperature
ρ=2.4×108Ωm\rho = 2.4 \times 10^{-8}\,\Omega\cdot\text{m}
Resistivity depends on temperature according to ρ=ρ0(1+αΔT)\rho = \rho_0(1 + \alpha \Delta T).
3
Calculate the total electrical resistance of the conductor
R = 2.4\,\Omega
Resistance is related to physical geometry and resistivity by R=ρLAR = \frac{\rho L}{A}.
4
Apply Ohm's law to solve for the current
I = 5.0\,\text{A}
Electric current is determined by potential difference divided by resistance (I=V/RI = V / R).

Key Concept

Temperature dependence of resistivity and Ohm's Law
Estimated Time:2m 0s
Question 911Question

A sample of ideal gas in a syringe occupies a volume of 300 cm3300\text{ cm}^3 at a temperature of 27C27^\circ\text{C}. If the pressure of the gas remains constant, what is its volume in cm3\text{cm}^3 when the temperature is raised to 127C127^\circ\text{C}?

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Answer: 400

Answer

400 cm³
According to Charles's Law, at constant pressure, the volume of a given mass of gas is directly proportional to its absolute temperature (VTV \propto T). Converting the given temperatures to kelvins yields T1=300 KT_1 = 300\text{ K} and T2=400 KT_2 = 400\text{ K}. Applying V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2} gives V2=300×400300=400 cm3V_2 = \frac{300 \times 400}{300} = 400\text{ cm}^3.

Step-by-Step Solution

1
Convert the initial and final temperatures from degrees Celsius to kelvins.
T1=27+273=300 KT_1 = 27 + 273 = 300\text{ K} and T2=127+273=400 KT_2 = 127 + 273 = 400\text{ K}
Gas law calculations require absolute temperature measured on the kelvin scale.
2
Apply Charles's Law, which relates volume and absolute temperature at constant pressure.
V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2}
The pressure of the gas is maintained constant.
3
Substitute the values into the equation and solve for the final volume V2V_2.
300 cm3300 K=V2400 K    V2=400 cm3\frac{300\text{ cm}^3}{300\text{ K}} = \frac{V_2}{400\text{ K}} \implies V_2 = 400\text{ cm}^3
Cross-multiplying gives V2=300×400300=400 cm3V_2 = \frac{300 \times 400}{300} = 400\text{ cm}^3.

Key Concept

Charles's Law
Question 912Question

A uniform conductor of length 4.0m4.0\,\text{m} and cross-sectional area 2.0×107m22.0 \times 10^{-7}\,\text{m}^2 has an electrical resistance of 0.50Ω0.50\,\Omega. What is the electrical resistivity of the material of the conductor in units of 108Ωm10^{-8}\,\Omega\cdot\text{m}?

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Answer: 2.5

Answer

The electrical resistivity of the material is 2.5×108Ωm2.5 \times 10^{-8}\,\Omega\cdot\text{m}, which gives a numerical value of 2.52.5 in units of 108Ωm10^{-8}\,\Omega\cdot\text{m}.
The electrical resistance RR of a conductor is given by R=ρLAR = \frac{\rho L}{A}, where ρ\rho is the resistivity, LL is the length, and AA is the cross-sectional area. Rearranging to solve for resistivity yields ρ=RAL\rho = \frac{R \cdot A}{L}. Substituting R=0.50ΩR = 0.50\,\Omega, A=2.0×107m2A = 2.0 \times 10^{-7}\,\text{m}^2, and L=4.0mL = 4.0\,\text{m} gives ρ=0.50×2.0×1074.0=2.5×108Ωm\rho = \frac{0.50 \times 2.0 \times 10^{-7}}{4.0} = 2.5 \times 10^{-8}\,\Omega\cdot\text{m}. Expressed in units of 108Ωm10^{-8}\,\Omega\cdot\text{m}, the answer is 2.52.5.

Step-by-Step Solution

1
Identify the relevant formula linking resistance, resistivity, length, and area.
R=ρLAR = \frac{\rho L}{A}
The resistance of a uniform conductor is directly proportional to its length and inversely proportional to its cross-sectional area.
2
Rearrange the equation to solve for resistivity ρ\rho.
ρ=RAL\rho = \frac{R \cdot A}{L}
Isolating ρ\rho allows direct evaluation using the given quantitative values.
3
Substitute the known numerical values into the equation.
ρ=0.50×(2.0×107)4.0=2.5×108Ωm\rho = \frac{0.50 \times (2.0 \times 10^{-7})}{4.0} = 2.5 \times 10^{-8}\,\Omega\cdot\text{m}
Performing the algebraic calculation gives the resistivity in SI units.

Key Concept

Electrical Resistivity and Conductor Dimensions
Question 913Question

A point P(x,y)P(x, y) moves in the Cartesian plane such that it is always equidistant from the two fixed points A(2,1)A(2, 1) and B(6,5)B(6, 5). If the locus of PP intersects the line 2x+y=142x + y = 14 at the point (x0,y0)(x_0, y_0), what is the value of x0x_0?

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Answer: 7

Answer

The value of x0x_0 is 77.
The locus of points equidistant from A(2,1)A(2, 1) and B(6,5)B(6, 5) is the perpendicular bisector of line segment ABAB. The midpoint of ABAB is (4,3)(4, 3) and its slope is 11, giving the perpendicular bisector a slope of 1-1. The equation of this locus is y3=1(x4)y - 3 = -1(x - 4), or x+y=7x + y = 7. Subtracting x+y=7x + y = 7 from 2x+y=142x + y = 14 directly gives x0=7x_0 = 7.

Step-by-Step Solution

1
Determine the equation of the locus of point P
The locus of P is the perpendicular bisector of segment AB, represented by x+y=7x + y = 7.
The set of all points equidistant from two fixed points forms the perpendicular bisector of the line segment connecting those points.
2
Find the point of intersection with the line 2x+y=142x + y = 14
Solving x+y=7x + y = 7 and 2x+y=142x + y = 14 simultaneously gives x0=7x_0 = 7.
The intersection point of two geometric lines must satisfy both equations simultaneously.

Key Concept

Perpendicular Bisector Locus and Line Intersections
Question 914Question

A 6.0 μF6.0\text{ }\mu\text{F} capacitor is charged to a potential difference of 100 V100\text{ V} using a direct-current source and then disconnected. It is subsequently connected in parallel across an uncharged 4.0 μF4.0\text{ }\mu\text{F} capacitor. What is the total electrostatic potential energy lost in the system during the redistribution of charge, in millijoules (mJ)?

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Answer: 12

Answer

The total electrostatic potential energy lost in the system during the redistribution of charge is 12 mJ.
The initial energy stored in the charged capacitor is Ui=12C1V12=12(6.0×106 F)(100 V)2=30 mJU_i = \frac{1}{2} C_1 V_1^2 = \frac{1}{2}(6.0 \times 10^{-6}\text{ F})(100\text{ V})^2 = 30\text{ mJ}. When connected in parallel to the uncharged capacitor, the total charge Q=600 μCQ = 600\text{ }\mu\text{C} is conserved across an equivalent capacitance of Ceq=6.0 μF+4.0 μF=10.0 μFC_{eq} = 6.0\text{ }\mu\text{F} + 4.0\text{ }\mu\text{F} = 10.0\text{ }\mu\text{F}. The common potential becomes Vf=QCeq=60 VV_f = \frac{Q}{C_{eq}} = 60\text{ V}, leading to a final stored energy Uf=12CeqVf2=18 mJU_f = \frac{1}{2} C_{eq} V_f^2 = 18\text{ mJ}. The energy lost is ΔU=UiUf=30 mJ18 mJ=12 mJ\Delta U = U_i - U_f = 30\text{ mJ} - 18\text{ mJ} = 12\text{ mJ}.

Step-by-Step Solution

1
Calculate the initial stored charge QQ and initial energy UiU_i in the charged 6.0 μF6.0\text{ }\mu\text{F} capacitor.
Q=6.0×104 C=600 μCQ = 6.0 \times 10^{-4}\text{ C} = 600\text{ }\mu\text{C} and Ui=3.0×102 J=30 mJU_i = 3.0 \times 10^{-2}\text{ J} = 30\text{ mJ}.
Before connection, all charge and energy reside solely on the first capacitor.
2
Find the equivalent capacitance CeqC_{eq} when the two capacitors are connected in parallel.
Ceq=6.0 μF+4.0 μF=10.0 μFC_{eq} = 6.0\text{ }\mu\text{F} + 4.0\text{ }\mu\text{F} = 10.0\text{ }\mu\text{F}.
Capacitances add directly when connected in parallel.
3
Determine the common final potential difference VfV_f across the combination.
Vf=QCeq=600 μC10.0 μF=60 VV_f = \frac{Q}{C_{eq}} = \frac{600\text{ }\mu\text{C}}{10.0\text{ }\mu\text{F}} = 60\text{ V}.
Total electric charge is conserved during redistribution between connected capacitors.
4
Calculate the final total energy UfU_f stored in the combined system.
Uf=12CeqVf2=12(10.0×106 F)(60 V)2=18 mJU_f = \frac{1}{2} C_{eq} V_f^2 = \frac{1}{2} (10.0 \times 10^{-6}\text{ F})(60\text{ V})^2 = 18\text{ mJ}.
Both capacitors now store energy under the new common potential difference.
5
Compute the total energy lost ΔU=UiUf\Delta U = U_i - U_f.
ΔU=30 mJ18 mJ=12 mJ\Delta U = 30\text{ mJ} - 18\text{ mJ} = 12\text{ mJ}.
The difference in energy is dissipated as heat in connecting wires and spark/radiation.

Key Concept

Charge Conservation and Energy Dissipation during Charge Sharing in Capacitors
Estimated Time:2m 0s
Question 915Question

An electron inside an excited gas atom undergoes a transition from an upper energy level of 2.40 eV-2.40\text{ eV} to a lower energy level of 5.15 eV-5.15\text{ eV}. What is the wavelength, in nanometers (nm\text{nm}), of the emitted photon? (Take Planck's constant h=6.6×1034 J sh = 6.6 \times 10^{-34}\text{ J s}, speed of light c=3.0×108 m s1c = 3.0 \times 10^8\text{ m s}^{-1}, and 1 eV=1.6×1019 J1\text{ eV} = 1.6 \times 10^{-19}\text{ J})

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Answer: 450

Answer

The wavelength of the emitted photon is 450 nm.
When an electron transitions from a higher energy level to a lower energy level, a photon is emitted with energy equal to the difference between the two energy states. Converting 2.75 eV to 4.40 x 10^-19 J and applying lambda = hc / E yields a wavelength of 4.50 x 10^-7 m, which equals 450 nm.

Step-by-Step Solution

1
Calculate the energy change of the transition in eV
\Delta E = -2.40\text{ eV} - (-5.15\text{ eV}) = 2.75\text{ eV}
The energy of the emitted photon equals the difference between the higher and lower electronic energy states.
2
Convert the transition energy into SI units (Joules)
\Delta E = 2.75 \times 1.6 \times 10^{-19}\text{ J} = 4.40 \times 10^{-19}\text{ J}
Standard physics constants h and c require energy to be expressed in Joules.
3
Calculate photon wavelength and convert to nanometers
\lambda = \frac{hc}{\Delta E} = \frac{1.98 \times 10^{-25}\text{ J m}}{4.40 \times 10^{-19}\text{ J}} = 4.50 \times 10^{-7}\text{ m} = 450\text{ nm}
Applying the de Broglie/Einstein relation connecting photon energy and wavelength.

Key Concept

Energy Level Transitions and Atomic Emission Spectra
Question 916Question

A galvanometer has an internal resistance of 19.0 Ω19.0\text{ }\Omega and produces a full-scale deflection for a current of 50 mA50\text{ mA}. What value of shunt resistance, in ohms (Ω\Omega), must be connected in parallel with the galvanometer to convert it into an ammeter capable of measuring currents up to 1.0 A1.0\text{ A}?

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Answer: 1

Answer

The required shunt resistance is 1.0 Ω1.0\text{ }\Omega.
To convert a sensitive galvanometer into an ammeter, a low-resistance resistor called a shunt (RsR_s) is connected in parallel with the galvanometer. This provides an alternative path for the bulk of the total current. Since the potential difference across parallel branches is equal, IsRs=IgRgI_s R_s = I_g R_g. Substituting Ig=0.05 AI_g = 0.05\text{ A}, Rg=19.0 ΩR_g = 19.0\text{ }\Omega, and Is=1.0 A0.05 A=0.95 AI_s = 1.0\text{ A} - 0.05\text{ A} = 0.95\text{ A} yields Rs=0.05×19.00.95=1.0 ΩR_s = \frac{0.05 \times 19.0}{0.95} = 1.0\text{ }\Omega.

Step-by-Step Solution

1
Convert the galvanometer full-scale deflection current IgI_g to amperes.
Ig=50 mA=0.05 AI_g = 50\text{ mA} = 0.05\text{ A}
Standard SI units must be used for electrical calculations.
2
Calculate the current IsI_s that must bypass the galvanometer through the shunt resistor.
Is=IIg=1.0 A0.05 A=0.95 AI_s = I - I_g = 1.0\text{ A} - 0.05\text{ A} = 0.95\text{ A}
By Kirchhoff's current law, the total maximum current splits into galvanometer current and shunt current.
3
Calculate the required shunt resistance RsR_s using the parallel voltage relation.
Rs=IgRgIs=0.05 A×19.0 Ω0.95 A=1.0 ΩR_s = \frac{I_g R_g}{I_s} = \frac{0.05\text{ A} \times 19.0\text{ }\Omega}{0.95\text{ A}} = 1.0\text{ }\Omega
Because the galvanometer and shunt resistor are connected in parallel, they share the exact same potential difference.

Key Concept

Galvanometer Conversion to Ammeter using a Shunt Resistor
Question 917Question

A cargo ship departs from port MM and sails 24 km24\text{ km} on a bearing of 050050^\circ to reach point NN. From point NN, the ship changes course and sails 10 km10\text{ km} on a bearing of 140140^\circ to reach point PP. What is the direct distance, in kilometers, from port MM to point PP?

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Answer: 26

Answer

The direct distance from port M to point P is 26 km.
The back bearing from N to M is 230°, and the bearing from N to P is 140°. The interior angle at N is 230° - 140° = 90°. Using the Pythagorean theorem for the right triangle formed by M, N, and P, the direct distance is √(24² + 10²) = √676 = 26 km.

Step-by-Step Solution

1
Calculate the interior angle MNP\angle MNP at point NN
MNP=(050+180)140=230140=90\angle MNP = (050^\circ + 180^\circ) - 140^\circ = 230^\circ - 140^\circ = 90^\circ
The back bearing from NN to MM is 230230^\circ. Subtracting the forward bearing to PP (140140^\circ) gives the enclosed interior angle.
2
Apply the Pythagorean theorem to right-angled triangle MNPMNP
MP=MN2+NP2=242+102=576+100=676=26 kmMP = \sqrt{MN^2 + NP^2} = \sqrt{24^2 + 10^2} = \sqrt{576 + 100} = \sqrt{676} = 26\text{ km}
Because MNP=90\angle MNP = 90^\circ, triangle MNPMNP is a right-angled triangle with hypotenuse MPMP.

Key Concept

Bearings and Right-Angled Triangles
Question 918Question

A Vernier caliper has 1010 divisions on its Vernier scale that coincide with 99 main scale divisions of 1 mm1\text{ mm} each. When the measuring jaws are fully closed without any object between them, the zero mark of the Vernier scale lies to the left of the main scale zero mark, and the 7th7\text{th} Vernier division coincides precisely with a main scale mark. When used to measure the internal diameter of a hollow brass ring, the main scale reads 3.5 cm3.5\text{ cm} and the 4th4\text{th} Vernier division coincides with a main scale mark. What is the actual corrected internal diameter of the ring in cm?

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Answer: 3.57

Answer

The corrected internal diameter of the hollow brass ring is 3.57 cm3.57\text{ cm}.
The least count of the Vernier caliper is 0.01 cm0.01\text{ cm}. The negative zero error is (107)×0.01 cm=0.03 cm-(10 - 7) \times 0.01\text{ cm} = -0.03\text{ cm}. The observed reading is 3.5 cm+(4×0.01 cm)=3.54 cm3.5\text{ cm} + (4 \times 0.01\text{ cm}) = 3.54\text{ cm}. Correcting for zero error gives 3.54 cm(0.03 cm)=3.57 cm3.54\text{ cm} - (-0.03\text{ cm}) = 3.57\text{ cm}.

Step-by-Step Solution

1
Calculate the least count of the Vernier caliper.
Least count = 0.01 cm0.01\text{ cm} (0.1 mm0.1\text{ mm}).
One main scale division is 1 mm=0.1 cm1\text{ mm} = 0.1\text{ cm}. Ten Vernier divisions equal nine main scale divisions (0.9 mm0.9\text{ mm}), so one Vernier division = 0.09 cm0.09\text{ cm}. Least count = 0.1 cm0.09 cm=0.01 cm0.1\text{ cm} - 0.09\text{ cm} = 0.01\text{ cm}.
2
Determine the zero error of the instrument.
Zero Error = 0.03 cm-0.03\text{ cm}.
For a negative zero error where the Vernier zero lies to the left of the main scale zero, Zero Error = (Nn)×least count-(N - n) \times \text{least count}, where N=10N = 10 and n=7n = 7. Thus, Zero Error = (107)×0.01 cm=0.03 cm-(10 - 7) \times 0.01\text{ cm} = -0.03\text{ cm}.
3
Calculate the uncorrected observed reading.
Observed Reading = 3.54 cm3.54\text{ cm}.
Observed Reading = Main scale reading + (Vernier coincided division \times Least count) = 3.5 cm+(4×0.01 cm)=3.54 cm3.5\text{ cm} + (4 \times 0.01\text{ cm}) = 3.54\text{ cm}.
4
Apply zero error correction to obtain the actual reading.
Corrected Reading = 3.57 cm3.57\text{ cm}.
Corrected Reading = Observed Reading - Zero Error = 3.54 cm(0.03 cm)=3.57 cm3.54\text{ cm} - (-0.03\text{ cm}) = 3.57\text{ cm}.

Key Concept

Measurement of length using a Vernier caliper with negative zero error correction
Question 919Question

A battery with an electromotive force (e.m.f.) of 12.0 V12.0\text{ V} and an internal resistance of 1.0 Ω1.0\text{ }\Omega is connected across a load resistor of 5.0 Ω5.0\text{ }\Omega. What is the terminal potential difference across the battery in volts?

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Answer: 10

Answer

The terminal potential difference across the battery is 10.0 V10.0\text{ V}.
The total resistance in the circuit is the sum of the external load resistance and the battery's internal resistance (Rtotal=5.0 Ω+1.0 Ω=6.0 ΩR_{\text{total}} = 5.0\text{ }\Omega + 1.0\text{ }\Omega = 6.0\text{ }\Omega). The current drawn from the battery is I=12.0 V6.0 Ω=2.0 AI = \frac{12.0\text{ V}}{6.0\text{ }\Omega} = 2.0\text{ A}. The terminal potential difference available to the external load is V=IR=2.0 A×5.0 Ω=10.0 VV = I \cdot R = 2.0\text{ A} \times 5.0\text{ }\Omega = 10.0\text{ V}.

Step-by-Step Solution

1
Find the total circuit resistance including internal resistance
Rtotal=5.0 Ω+1.0 Ω=6.0 ΩR_{\text{total}} = 5.0\text{ }\Omega + 1.0\text{ }\Omega = 6.0\text{ }\Omega
The internal resistance of the cell acts in series with the external load resistor.
2
Determine total current in the circuit
I=ERtotal=12.0 V6.0 Ω=2.0 AI = \frac{E}{R_{\text{total}}} = \frac{12.0\text{ V}}{6.0\text{ }\Omega} = 2.0\text{ A}
By Ohm's law, current equals total electromotive force divided by total circuit resistance.
3
Compute the terminal potential difference
V=I×R=2.0 A×5.0 Ω=10.0 VV = I \times R = 2.0\text{ A} \times 5.0\text{ }\Omega = 10.0\text{ V}
Terminal voltage is the voltage drop across the load resistor, equivalent to EIrE - I \cdot r.

Key Concept

Terminal Potential Difference and Internal Resistance
Question 920Question

In a cathode-ray tube, electrons of mass 9.10×1031 kg9.10 \times 10^{-31}\text{ kg} and elementary charge 1.60×1019 C1.60 \times 10^{-19}\text{ C} are accelerated from rest by the electric field between the cathode and the anode. What potential difference, in volts, is required to accelerate these electrons to a speed of 8.00×106 m s18.00 \times 10^{6}\text{ m s}^{-1}?

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Answer: 182

Answer

The potential difference required to accelerate the electrons to the specified speed is 182 V182\text{ V}.
The work done by an accelerating potential difference VV on an electron of charge ee is converted entirely into kinetic energy 12mv2\frac{1}{2} m v^2. Solving eV=12mv2e V = \frac{1}{2} m v^2 for VV yields V=mv22e=182 VV = \frac{m v^2}{2 e} = 182\text{ V}.

Step-by-Step Solution

1
Equate the work done by the electric field to the kinetic energy gained by an electron.
W=eV=12mv2W = e V = \frac{1}{2} m v^2
Work done on a charged particle moving through an electric potential difference equals its gain in kinetic energy.
2
Isolate the potential difference VV on one side of the equation.
V=mv22eV = \frac{m v^2}{2 e}
Algebraic rearrangement to solve for the target variable.
3
Substitute the given numerical parameters into the equation.
V=(9.10×1031 kg)×(8.00×106 m s1)22×(1.60×1019 C)V = \frac{(9.10 \times 10^{-31}\text{ kg}) \times (8.00 \times 10^{6}\text{ m s}^{-1})^2}{2 \times (1.60 \times 10^{-19}\text{ C})}
Populating the formula with the specified values for electron mass, speed, and charge.
4
Perform the final calculation.
V=182 VV = 182\text{ V}
Simplifying the numerical expression gives 182 V182\text{ V}.

Key Concept

Acceleration of charged particles in electric fields
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