Tüm alıştırma soruları

1526 soru

Soru 941Soru

A radioactive mixture initially contains two radioisotopes, PP and QQ, such that the initial number of undecayed nuclei of PP is 88 times that of QQ. If the half-life of isotope PP is 2 hours2\text{ hours} and the half-life of isotope QQ is 6 hours6\text{ hours}, calculate the time, in hours, after which the number of undecayed nuclei of both isotopes will be equal.

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Cevap: 9

Cevap

The time after which the number of undecayed nuclei of both isotopes will be equal is 9 hours.
By applying the radioactive decay law N(t)=N0(1/2)t/T1/2N(t) = N_0(1/2)^{t/T_{1/2}} to both isotopes with initial ratio NP0=8NQ0N_{P0} = 8N_{Q0} and equating NP(t)=NQ(t)N_P(t) = N_Q(t), we obtain 8=2t/38 = 2^{t/3}, which gives t=9 hourst = 9\text{ hours}.

Adım Adım Çözüm

1
Write the decay equations for isotopes P and Q based on their half-lives
NP(t)=NP0(12)t/2N_P(t) = N_{P0}\left(\frac{1}{2}\right)^{t/2} and NQ(t)=NQ0(12)t/6N_Q(t) = N_{Q0}\left(\frac{1}{2}\right)^{t/6}
Radioactive decay follows the exponential relationship N(t)=N0(12)t/T1/2N(t) = N_0 \left(\frac{1}{2}\right)^{t/T_{1/2}}.
2
Apply the initial condition NP0=8NQ0N_{P0} = 8 N_{Q0} and set the two expressions equal
8NQ0(12)t/2=NQ0(12)t/68 N_{Q0} \left(\frac{1}{2}\right)^{t/2} = N_{Q0} \left(\frac{1}{2}\right)^{t/6}
The problem asks for the time tt when both isotopes have equal remaining undecayed nuclei.
3
Divide both sides by NQ0(12)t/2N_{Q0} \left(\frac{1}{2}\right)^{t/2} and simplify the exponents
8=(1/2)t/6(1/2)t/2=(12)t/3=2t/38 = \frac{(1/2)^{t/6}}{(1/2)^{t/2}} = \left(\frac{1}{2}\right)^{-t/3} = 2^{t/3}
Applying exponent laws simplifies the ratio of powers of one-half into a single base-two exponent.
4
Solve for time tt using powers of 2
23=2t/3    t3=3    t=9 hours2^3 = 2^{t/3} \implies \frac{t}{3} = 3 \implies t = 9\text{ hours}
Equating the exponents of identical base 2 gives the exact time.

Anahtar Kavram

Radioactive Decay Law and Half-life for Isotope Mixtures
Tahmini Süre:2m 0s
Soru 942Soru

A 250 dm3250\text{ dm}^3 sample of hard water contains 0.012 mol dm30.012\text{ mol dm}^{-3} of dissolved magnesium tetraoxosulfate(VI), MgSO4\text{MgSO}_4. What mass, in grams, of anhydrous sodium trioxocarbonate(IV), Na2CO3\text{Na}_2\text{CO}_3, is required to completely precipitate all the magnesium ions as magnesium trioxocarbonate(IV) and soften the water? [Molar mass of Na2CO3=106 g mol1][\text{Molar mass of Na}_2\text{CO}_3 = 106\text{ g mol}^{-1}]

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Cevap: 318

Cevap

318 g of anhydrous sodium trioxocarbonate(IV) is required.
Permanent water hardness caused by soluble magnesium salts like magnesium tetraoxosulfate(VI) (MgSO4\text{MgSO}_4) is removed by reaction with sodium trioxocarbonate(IV) (Na2CO3\text{Na}_2\text{CO}_3). The balanced reaction MgSO4(aq)+Na2CO3(aq)MgCO3(s)+Na2SO4(aq)\text{MgSO}_4\text{(aq)} + \text{Na}_2\text{CO}_3\text{(aq)} \rightarrow \text{MgCO}_3\text{(s)} + \text{Na}_2\text{SO}_4\text{(aq)} shows a 1:1 molar ratio. A 250 dm3250\text{ dm}^3 volume at 0.012 mol dm30.012\text{ mol dm}^{-3} contains 3.0 moles3.0\text{ moles} of MgSO4\text{MgSO}_4, which requires 3.0 moles3.0\text{ moles} of Na2CO3\text{Na}_2\text{CO}_3. Multiplying by its molar mass (106 g mol1106\text{ g mol}^{-1}) gives 318 g318\text{ g}.

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1
Calculate the total number of moles of magnesium tetraoxosulfate(VI) in the water sample.
n(MgSO4)=250 dm3×0.012 mol dm3=3.0 moln(\text{MgSO}_4) = 250\text{ dm}^3 \times 0.012\text{ mol dm}^{-3} = 3.0\text{ mol}
Molar amount is calculated by multiplying the solution volume by its molar concentration.
2
Write the balanced chemical equation for softening permanent hardness with sodium trioxocarbonate(IV).
MgSO4(aq)+Na2CO3(aq)MgCO3(s)+Na2SO4(aq)\text{MgSO}_4(\text{aq}) + \text{Na}_2\text{CO}_3(\text{aq}) \rightarrow \text{MgCO}_3(\text{s}) + \text{Na}_2\text{SO}_4(\text{aq})
Soluble magnesium ions causing permanent hardness are removed by precipitation as insoluble magnesium trioxocarbonate(IV).
3
Calculate the mass of anhydrous sodium trioxocarbonate(IV) needed.
Mass=3.0 mol×106 g mol1=318 g\text{Mass} = 3.0\text{ mol} \times 106\text{ g mol}^{-1} = 318\text{ g}
From the 1:1 stoichiometric ratio, 3.0 moles of sodium trioxocarbonate(IV) is required.

Anahtar Kavram

Quantitative removal of permanent water hardness using sodium trioxocarbonate(IV) (washing soda)
Soru 943Soru

A non-uniform wooden pole of length 6.0 m6.0\text{ m} and weight 150 N150\text{ N} is balanced horizontally on a pivot placed 2.4 m2.4\text{ m} from its heavy end PP. The system achieves rotational equilibrium when a load of 50 N50\text{ N} is hung directly from end PP. What is the distance of the center of gravity of the pole from end PP?

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Cevap: 3.2

Cevap

The distance of the center of gravity of the pole from end PP is 3.2 m3.2\text{ m}.
Taking moments about the pivot at 2.4 m2.4\text{ m} from end PP, the counter-clockwise moment created by the 50 N50\text{ N} load (50 N×2.4 m=120 Nm50\text{ N} \times 2.4\text{ m} = 120\text{ N}\cdot\text{m}) must balance the clockwise moment created by the 150 N150\text{ N} weight of the pole acting at its center of gravity (150 N×(d2.4 m)150\text{ N} \times (d - 2.4\text{ m})). Equating these gives 120=150(d2.4)120 = 150(d - 2.4), leading to d2.4=0.8 md - 2.4 = 0.8\text{ m}, so d=3.2 md = 3.2\text{ m}.

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1
Identify force positions relative to the pivot
The 50 N50\text{ N} load is 2.4 m2.4\text{ m} to the left of the pivot. The 150 N150\text{ N} weight acts at the center of gravity, which is (d2.4 m)(d - 2.4\text{ m}) to the right of the pivot.
Moments are evaluated relative to the fulcrum to eliminate the unknown normal reaction force at the pivot.
2
Apply the Principle of Moments
Anti-clockwise moment = 50×2.4=120 Nm50 \times 2.4 = 120\text{ N}\cdot\text{m}. Clockwise moment = 150×(d2.4)150 \times (d - 2.4). Setting them equal: 120=150(d2.4)120 = 150(d - 2.4).
For a body in rotational equilibrium, the total clockwise moment about any pivot equals the total anti-clockwise moment.
3
Solve the equation for distance dd
d2.4=0.8    d=3.2 md - 2.4 = 0.8 \implies d = 3.2\text{ m}.
Adding the displacement from the pivot (0.8 m0.8\text{ m}) to the pivot position from end PP (2.4 m2.4\text{ m}) yields the position of the center of gravity from end PP.

Anahtar Kavram

Rotational equilibrium and Principle of Moments for non-uniform rigid bodies
Tahmini Süre:1m 30s
Soru 944Soru

A 4.00 g4.00\text{ g} sample of a copper oxide is completely reduced by dry hydrogen gas to yield 3.20 g3.20\text{ g} of metallic copper. According to the Law of Definite Proportions, what mass of this same copper oxide, in grams, will be produced when 5.00 g5.00\text{ g} of pure copper is completely oxidized?

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Cevap: 6.25

Cevap

6.25 g
According to the Law of Definite Proportions (or Constant Composition), a chemical compound always contains its component elements in fixed mass ratios. In the first sample, copper makes up 3.20 g/4.00 g=0.803.20\text{ g} / 4.00\text{ g} = 0.80 or 80%80\% of the total mass. Therefore, in any sample of this oxide, 5.00 g5.00\text{ g} of copper represents 80%80\% of the total mass. Dividing 5.00 g5.00\text{ g} by 0.800.80 gives 6.25 g6.25\text{ g} of copper oxide.

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1
Determine the mass percentage (or mass fraction) of copper in the compound from the first experiment
Mass fraction of Cu = 3.20 / 4.00 = 0.80 (80%)
The first experiment provides quantitative data regarding the mass of copper contained in a known mass of oxide.
2
Apply the Law of Definite Proportions to calculate the required mass of copper oxide for 5.00 g of copper
Mass of Copper Oxide = 5.00 / 0.80 = 6.25 g
The Law of Definite Proportions dictates that the mass composition ratio remains constant regardless of the sample source or size.

Anahtar Kavram

Law of Definite Proportions
Soru 945Soru

A particle of mass 0.50 kg0.50\text{ kg} executes simple harmonic motion along a straight line. When its displacement from the equilibrium position is 0.06 m0.06\text{ m}, its speed is 0.80 m/s0.80\text{ m/s} and its potential energy is 0.09 J0.09\text{ J}. What is the magnitude of the maximum acceleration of the particle in m/s2\text{m/s}^2?

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Cevap: 10

Cevap

The magnitude of the maximum acceleration of the particle is 10 m/s210\text{ m/s}^2.
Using potential energy Ep=12mω2x2E_p = \frac{1}{2}m\omega^2 x^2, the angular frequency ω\omega is 10 rad/s10\text{ rad/s}. Using v=ωA2x2v = \omega\sqrt{A^2 - x^2}, the amplitude AA is 0.10 m0.10\text{ m}. Substituting these values into amax=ω2Aa_{\max} = \omega^2 A yields 10 m/s210\text{ m/s}^2.

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1
Find angular frequency ω\omega from potential energy.
ω=10 rad/s\omega = 10\text{ rad/s}
Using potential energy Ep=12mω2x2E_p = \frac{1}{2}m\omega^2 x^2: 0.09=12(0.50)ω2(0.06)2    0.09=0.0009ω2    ω2=100    ω=10 rad/s0.09 = \frac{1}{2}(0.50)\omega^2 (0.06)^2 \implies 0.09 = 0.0009 \omega^2 \implies \omega^2 = 100 \implies \omega = 10\text{ rad/s}.
2
Find amplitude AA from speed.
A=0.10 mA = 0.10\text{ m}
Using speed v=ωA2x2v = \omega\sqrt{A^2 - x^2}: 0.80=10A20.062    0.08=A20.0036    0.0064=A20.0036    A2=0.0100    A=0.10 m0.80 = 10\sqrt{A^2 - 0.06^2} \implies 0.08 = \sqrt{A^2 - 0.0036} \implies 0.0064 = A^2 - 0.0036 \implies A^2 = 0.0100 \implies A = 0.10\text{ m}.
3
Calculate maximum acceleration.
amax=10 m/s2a_{\max} = 10\text{ m/s}^2
Using maximum acceleration formula amax=ω2Aa_{\max} = \omega^2 A: amax=100×0.10=10 m/s2a_{\max} = 100 \times 0.10 = 10\text{ m/s}^2.

Anahtar Kavram

Simple Harmonic Motion Energy and Kinematic Relations
Soru 946Soru

When a 2.0 g2.0\text{ g} sample of a solid solute is completely dissolved in 100.0 g100.0\text{ g} of distilled water initially at 25.0C25.0^\circ\text{C}, an exothermic process occurs and the temperature of the water rises to 30.0C30.0^\circ\text{C}. Assuming the specific heat capacity of water is 4.2 J g1 K14.2\text{ J g}^{-1}\text{ K}^{-1} and neglecting the heat capacity of the calorimeter container, what is the amount of heat energy, in Joules, absorbed by the water?

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Cevap: 2100

Cevap

The amount of heat energy absorbed by the water is 2100 J2100\text{ J}.
In an exothermic process, heat is transferred to the surroundings (water). Using the calorimetric relation Q=mcΔTQ = m c \Delta T with m=100.0 gm = 100.0\text{ g}, c=4.2 J g1 K1c = 4.2\text{ J g}^{-1}\text{ K}^{-1}, and ΔT=(30.025.0) K=5.0 K\Delta T = (30.0 - 25.0)\text{ K} = 5.0\text{ K}, the heat gained by the water is Q=100.0×4.2×5.0=2100 JQ = 100.0 \times 4.2 \times 5.0 = 2100\text{ J}.

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1
Determine the change in temperature (ΔT\Delta T) of the water.
ΔT=TfinalTinitial=30.0C25.0C=5.0C=5.0 K\Delta T = T_{\text{final}} - T_{\text{initial}} = 30.0^\circ\text{C} - 25.0^\circ\text{C} = 5.0^\circ\text{C} = 5.0\text{ K}
The heat calculation requires the temperature difference resulting from the exothermic dissolution.
2
Apply the heat formula Q=mcΔTQ = m c \Delta T.
Q=100.0 g×4.2 J g1 K1×5.0 KQ = 100.0\text{ g} \times 4.2\text{ J g}^{-1}\text{ K}^{-1} \times 5.0\text{ K}
Heat absorbed depends directly on the mass of water, its specific heat capacity, and the temperature rise.
3
Calculate the total heat energy absorbed.
Q=2100 JQ = 2100\text{ J}
Multiplying the mass, heat capacity, and temperature change yields 2100 J2100\text{ J}.

Anahtar Kavram

Calorimetric Heat Calculation (Q=mcΔTQ = m c \Delta T)
Soru 947Soru

Heavy water is water in which the hydrogen atoms are replaced by the hydrogen isotope deuterium (12H^{2}_{1}\text{H} or D\text{D}). Given that the atomic mass of deuterium is 2 g mol12\text{ g mol}^{-1} and oxygen (816O^{16}_{8}\text{O}) is 16 g mol116\text{ g mol}^{-1}, what is the molar mass of heavy water (D2O\text{D}_2\text{O}) in g mol1\text{g mol}^{-1}?

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Cevap: 20

Cevap

The molar mass of heavy water (D2O\text{D}_2\text{O}) is 20 g mol120\text{ g mol}^{-1}.
Heavy water (D2O\text{D}_2\text{O}) contains two atoms of deuterium (2H^2\text{H}, atomic mass = 22) and one atom of oxygen (16O^{16}\text{O}, atomic mass = 1616). The molar mass is calculated as (2×2)+16=20 g mol1(2 \times 2) + 16 = 20\text{ g mol}^{-1}.

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1
Determine the molecular composition of heavy water
Heavy water (D2O\text{D}_2\text{O}) contains 2 deuterium atoms and 1 oxygen atom.
Deuterium is an isotope of hydrogen containing one proton and one neutron, giving it a mass number of 2.
2
Sum the relative atomic masses of all constituent atoms
(2×2)+16=20 g mol1(2 \times 2) + 16 = 20\text{ g mol}^{-1}
Multiplying the mass of deuterium by two and adding the mass of one oxygen atom yields the molar mass of the compound.

Anahtar Kavram

Heavy Water and Deuterium Molar Mass
Soru 948Soru

A particle of mass 0.20 kg0.20\text{ kg} executes simple harmonic motion along a straight line. When its displacement from the equilibrium position is 0.03 m0.03\text{ m}, its speed is 0.16 m/s0.16\text{ m/s}. When its displacement is 0.04 m0.04\text{ m}, its speed is 0.12 m/s0.12\text{ m/s}. What is the total mechanical energy of the particle in millijoules (mJ\text{mJ})?

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Cevap: 4

Cevap

The total mechanical energy of the particle is 4 mJ4\text{ mJ}.
Using the relation v2=ω2(A2x2)v^2 = \omega^2(A^2 - x^2) for the two given state points (0.03 m,0.16 m/s)(0.03\text{ m}, 0.16\text{ m/s}) and (0.04 m,0.12 m/s)(0.04\text{ m}, 0.12\text{ m/s}) forms a set of simultaneous equations. Subtracting them yields ω2=16 rad2/s2\omega^2 = 16\text{ rad}^2/\text{s}^2, leading to A2=0.0025 m2A^2 = 0.0025\text{ m}^2. Substituting these values into E=12mω2A2E = \frac{1}{2}m\omega^2 A^2 gives E=0.004 JE = 0.004\text{ J}, which converts to 4 mJ4\text{ mJ}.

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1
Set up kinematic equations for both displacement points using v2=ω2(A2x2)v^2 = \omega^2(A^2 - x^2).
0.0256=ω2(A20.0009)0.0256 = \omega^2(A^2 - 0.0009) and 0.0144=ω2(A20.0016)0.0144 = \omega^2(A^2 - 0.0016).
The equation relates linear speed, angular frequency, amplitude, and instantaneous displacement in SHM.
2
Subtract the two simultaneous equations to eliminate A2A^2 and find ω2\omega^2.
0.0112=0.0007ω2    ω2=16 rad2/s20.0112 = 0.0007\omega^2 \implies \omega^2 = 16\text{ rad}^2/\text{s}^2.
Eliminating amplitude isolates the angular frequency squared.
3
Determine A2A^2 by substituting ω2=16\omega^2 = 16 back into one of the state equations.
A2=0.0025 m2    A=0.05 mA^2 = 0.0025\text{ m}^2 \implies A = 0.05\text{ m}.
Amplitude is required to calculate the maximum potential or total mechanical energy.
4
Calculate total mechanical energy E=12mω2A2E = \frac{1}{2}m\omega^2 A^2 and convert to millijoules.
E=12×0.20×16×0.0025=0.004 J=4 mJE = \frac{1}{2} \times 0.20 \times 16 \times 0.0025 = 0.004\text{ J} = 4\text{ mJ}.
Total energy in SHM is constant and proportional to mass, square of angular frequency, and square of amplitude.

Anahtar Kavram

Conservation of energy and phase-space relationship between velocity and displacement in simple harmonic motion.
Soru 949Soru

A small spherical lead shot of radius 3.0×103 m3.0 \times 10^{-3}\text{ m} and density 8000 kg/m38000\text{ kg/m}^3 falls vertically through a viscous oil of density 800 kg/m3800\text{ kg/m}^3 and dynamic viscosity 0.18 Pas0.18\text{ Pa}\cdot\text{s}. What is the magnitude of the terminal velocity of the sphere in m/s\text{m/s}? (Take g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 0.8

Cevap

The terminal velocity of the lead shot is 0.8 m/s0.8\text{ m/s}.
At terminal velocity, acceleration is zero because the upward forces (viscous drag 6πηrvt6\pi \eta r v_t plus buoyant upthrust 43πr3ρfg\frac{4}{3}\pi r^3 \rho_f g) completely balance the downward weight of the sphere (43πr3ρsg\frac{4}{3}\pi r^3 \rho_s g). Solving for velocity gives vt=2r2(ρsρf)g9η=0.8 m/sv_t = \frac{2 r^2 (\rho_s - \rho_f) g}{9 \eta} = 0.8\text{ m/s}.

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1
Formulate the force balance equation at terminal velocity.
Weight (WW) = Upthrust (UU) + Viscous drag (FvF_v), which simplifies to vt=2r2(ρsρf)g9ηv_t = \frac{2 r^2 (\rho_s - \rho_f) g}{9 \eta}.
When terminal velocity is attained, the net acceleration of the sphere is zero, so upward forces balance downward force.
2
Substitute the physical parameters into the terminal velocity formula.
vt=2×(3.0×103)2×(8000800)×109×0.18=0.8 m/sv_t = \frac{2 \times (3.0 \times 10^{-3})^2 \times (8000 - 800) \times 10}{9 \times 0.18} = 0.8\text{ m/s}.
Direct calculation using Stokes' law and Archimedes' principle.

Anahtar Kavram

Terminal Velocity and Stokes' Law in a Viscous Medium
Soru 950Soru

A uniform horizontal rod ABAB of length 2.0 m2.0\text{ m} and mass 6.0 kg6.0\text{ kg} is suspended horizontally by two light vertical strings attached at end AA and at a point CC located 0.5 m0.5\text{ m} from end BB. Taking g=10 m/s2g = 10\text{ m/s}^2, what is the tension in the string at point CC in Newtons?

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Cevap: 40

Cevap

The tension in the string at point C is 40 N.
The weight of the rod (60 N60\text{ N}) acts at its midpoint (1.0 m1.0\text{ m} from end AA). Point CC is located 1.5 m1.5\text{ m} from end AA. Taking moments about end AA gives 60 N×1.0 m=TC×1.5 m60\text{ N} \times 1.0\text{ m} = T_C \times 1.5\text{ m}, which evaluates to TC=40 NT_C = 40\text{ N}.

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1
Calculate total weight and identify the center of gravity position
Weight W=60 NW = 60\text{ N} acting at 1.0 m1.0\text{ m} from end AA
For a uniform rod, the weight acts vertically downwards at its geometric center.
2
Set up the moment equilibrium equation taking end A as pivot
60 N×1.0 m=TC×1.5 m60\text{ N} \times 1.0\text{ m} = T_C \times 1.5\text{ m}
Taking moments about point AA eliminates the force at AA and equates clockwise moment from weight to counter-clockwise moment from tension at CC.
3
Solve for the tension force at point C
TC=40 NT_C = 40\text{ N}
Dividing the total moment of 60 Nm60\text{ N}\cdot\text{m} by the moment arm of 1.5 m1.5\text{ m} yields 40 N40\text{ N}.

Anahtar Kavram

Principle of Moments and Rotational Equilibrium
Tahmini Süre:1m 30s
Soru 951Soru

A sample of a radioactive isotope has an initial activity of 8000 Bq8000\text{ Bq}. After an elapsed time of 18 minutes18\text{ minutes}, its activity reduces to 1000 Bq1000\text{ Bq}. Calculate the decay constant λ\lambda of the isotope in min1\text{min}^{-1}.

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Cevap: 0.1155

Cevap

The decay constant of the radioactive isotope is 0.1155 min10.1155\text{ min}^{-1}.
The activity decreases from 8000 Bq8000\text{ Bq} to 1000 Bq1000\text{ Bq}, which is a reduction to 18\frac{1}{8} of its initial value. Since (12)3=18\left(\frac{1}{2}\right)^3 = \frac{1}{8}, exactly 33 half-lives have elapsed in 18 minutes18\text{ minutes}, meaning T1/2=6 minutesT_{1/2} = 6\text{ minutes}. Using the relationship λ=ln2T1/2=0.693156 min\lambda = \frac{\ln 2}{T_{1/2}} = \frac{0.69315}{6\text{ min}}, we obtain λ0.1155 min1\lambda \approx 0.1155\text{ min}^{-1}.

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1
Determine the number of elapsed half-lives from the activity reduction ratio.
The fraction of remaining activity is AA0=10008000=18=(12)3\frac{A}{A_0} = \frac{1000}{8000} = \frac{1}{8} = \left(\frac{1}{2}\right)^3, giving n=3n = 3 half-lives.
Radioactive decay follows the relation A=A0(1/2)nA = A_0 (1/2)^n.
2
Determine the half-life T1/2T_{1/2} of the isotope.
T1/2=tn=18 min3=6 minutesT_{1/2} = \frac{t}{n} = \frac{18\text{ min}}{3} = 6\text{ minutes}.
Total elapsed time is equal to the number of half-lives multiplied by the duration of one half-life.
3
Compute the decay constant λ\lambda in min1\text{min}^{-1}.
λ=ln2T1/2=0.693156 min=0.1155 min1\lambda = \frac{\ln 2}{T_{1/2}} = \frac{0.69315}{6\text{ min}} = 0.1155\text{ min}^{-1}.
The decay constant is fundamental to decay rate and related to half-life via λ=ln2T1/2\lambda = \frac{\ln 2}{T_{1/2}}.

Anahtar Kavram

Radioactive Decay Law and Decay Constant
Tahmini Süre:2m 0s
Soru 952Soru

A composite cylindrical bar consists of two uniform sections of equal length joined end-to-end. Section A has a radius of 2.0 cm2.0\text{ cm} and a thermal conductivity of 300 W m1K1300\text{ W m}^{-1}\text{K}^{-1}. Section B has a radius of 4.0 cm4.0\text{ cm} and a thermal conductivity of 150 W m1K1150\text{ W m}^{-1}\text{K}^{-1}. The outer end of Section A is maintained at a constant temperature of 120C120^\circ\text{C}, while the outer end of Section B is held at 0C0^\circ\text{C}. Assuming the curved surfaces of both sections are perfectly insulated and heat flow is steady, what is the temperature at the junction between the two sections in C^\circ\text{C}?

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Cevap: 40

Cevap

The steady-state temperature at the junction between Section A and Section B is 40.0°C.
At steady state, the rate of heat conduction through Section A equals that through Section B. Because Section B has double the radius of Section A, its cross-sectional area is four times as large. Equating the heat flow rates gives 300 * A_A * (120 - T_J) = 150 * (4 A_A) * T_J, which simplifies directly to 120 - T_J = 2 T_J, yielding a junction temperature of 40.0°C.

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1
Determine the relationship between the cross-sectional areas of Section A and Section B.
The area ratio A_B / A_A = (r_B / r_A)² = (4.0 cm / 2.0 cm)² = 4.
The cross-sectional area of a cylinder is proportional to the square of its radius.
2
Write the steady-state heat flow equation for each section.
H_A = (k_A * A_A * (120 - T_J)) / L and H_B = (k_B * A_B * (T_J - 0)) / L.
According to Fourier's law of thermal conduction, the heat transfer rate through a uniform layer is proportional to thermal conductivity, cross-sectional area, and temperature difference, and inversely proportional to length.
3
Equate the heat transfer rates H_A and H_B and solve for the junction temperature T_J.
300 * A_A * (120 - T_J) = 150 * (4 A_A) * T_J => 300 * (120 - T_J) = 600 * T_J => 120 - T_J = 2 T_J => 3 T_J = 120 => T_J = 40.0°C.
At steady state with insulated sides, heat does not accumulate or escape, so the rate of heat conduction through both sections must be identical.

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Steady-state thermal conduction through composite conductors with differing cross-sectional areas and thermal conductivities
Soru 953Soru

An alternating current (AC) circuit contains an inductor of inductance L=0.2π2 HL = \frac{0.2}{\pi^2}\ \text{H}, a resistor of resistance R=40 ΩR = 40\ \Omega, and a variable capacitor CC connected in series across a 50 Hz50\ \text{Hz} voltage supply. What capacitance CC, in microfarads (μF\mu\text{F}), is required for the circuit to operate at electrical resonance?

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Cevap: 500

Cevap

The capacitance required to achieve electrical resonance is 500 μF.
At electrical resonance in a series RLC circuit, the inductive reactance (XLX_L) equals the capacitive reactance (XCX_C). Setting 2πfL=12πfC2\pi f L = \frac{1}{2\pi f C} yields f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}. Substituting f0=50 Hzf_0 = 50\ \text{Hz} and L=0.2π2 HL = \frac{0.2}{\pi^2}\ \text{H} into this equation gives C=5×104 FC = 5 \times 10^{-4}\ \text{F}, which equals 500 μF500\ \mu\text{F}.

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1
Recall the resonant frequency formula for a series RLC circuit.
f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}
At resonance, inductive reactance equals capacitive reactance (XL=XCX_L = X_C).
2
Substitute the given numerical parameters into the equation.
50=12π0.2π2C50 = \frac{1}{2\pi \sqrt{\frac{0.2}{\pi^2} \cdot C}}
Given frequency f0=50 Hzf_0 = 50\ \text{Hz} and inductance L=0.2π2 HL = \frac{0.2}{\pi^2}\ \text{H}.
3
Isolate the square root term and simplify.
0.2C=0.01\sqrt{0.2 C} = 0.01
Simplifying 2π1π=22\pi \cdot \frac{1}{\pi} = 2 and rearranging 20.2C=150=0.022 \sqrt{0.2 C} = \frac{1}{50} = 0.02.
4
Square both sides and solve for CC in farads.
C=5×104 FC = 5 \times 10^{-4}\ \text{F}
0.2C=(0.01)2=1040.2 C = (0.01)^2 = 10^{-4}, so C=1040.2=5×104 FC = \frac{10^{-4}}{0.2} = 5 \times 10^{-4}\ \text{F}.
5
Convert capacitance from farads to microfarads.
C=500 μFC = 500\ \mu\text{F}
Multiply farads by 10610^6 to express the result in microfarads.

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Resonant Frequency in Series AC Circuits
Soru 954Soru

An RLC series circuit operating at resonance contains an inductor of inductance 0.1 H0.1\text{ H} and a capacitor of capacitance 10 μF10\ \mu\text{F}. What is the resonant angular frequency of the circuit in radians per second (rad/s\text{rad/s})?

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Cevap: 1000

Cevap

The resonant angular frequency of the circuit is 1000 rad/s1000\text{ rad/s}.
The resonant angular frequency ω0\omega_0 of an AC circuit is determined by the formula ω0=1LC\omega_0 = \frac{1}{\sqrt{LC}}. Substituting the given values L=0.1 HL = 0.1\text{ H} and C=105 FC = 10^{-5}\text{ F} gives ω0=1106=1000 rad/s\omega_0 = \frac{1}{\sqrt{10^{-6}}} = 1000\text{ rad/s}.

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1
Convert given parameters to standard SI units
L=0.1 HL = 0.1\text{ H} and C=10×106 F=105 FC = 10 \times 10^{-6}\text{ F} = 10^{-5}\text{ F}.
Calculations must be performed in base SI units for dimensional consistency.
2
Calculate the resonant angular frequency using ω0=1LC\omega_0 = \frac{1}{\sqrt{LC}}
ω0=10.1×105=1106=1000 rad/s\omega_0 = \frac{1}{\sqrt{0.1 \times 10^{-5}}} = \frac{1}{\sqrt{10^{-6}}} = 1000\text{ rad/s}.
At resonance, inductive reactance equals capacitive reactance (XL=XCX_L = X_C), which yields ω0=1LC\omega_0 = \frac{1}{\sqrt{LC}}.

Anahtar Kavram

Resonant Angular Frequency
Soru 955Soru

A U-tube open to the atmosphere at both ends contains water of density 1000 kg m31000\text{ kg m}^{-3}. An immiscible liquid is poured into one arm of the tube until it forms a column of height 15.0 cm15.0\text{ cm}. If the interface between the two liquids lies 12.0 cm12.0\text{ cm} below the surface of the water in the opposite arm, what is the density of the liquid in kg m3\text{kg m}^{-3}?

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Cevap: 800

Cevap

The density of the immiscible liquid is 800 kg m3800\text{ kg m}^{-3}.
At the level of the liquid interface, the hydrostatic pressure exerted by the 15.0 cm15.0\text{ cm} liquid column must equal the hydrostatic pressure exerted by the 12.0 cm12.0\text{ cm} water column above it. Equating ρ1h1=ρ2h2\rho_1 h_1 = \rho_2 h_2 yields ρliquid=1000×(12.0/15.0)=800 kg m3\rho_{\text{liquid}} = 1000 \times (12.0 / 15.0) = 800\text{ kg m}^{-3}.

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1
Apply the principal of equal pressure at the same horizontal level in a continuous fluid at rest.
Pressure due to liquid column equals pressure due to water column above the interface line.
Hydrostatic pressure at depth hh is given by P=ρghP = \rho g h, and points at equal depth in a connected liquid body share identical pressure.
2
Set up the density-height ratio relationship: ρliquidhliquid=ρwaterhwater\rho_{\text{liquid}} \cdot h_{\text{liquid}} = \rho_{\text{water}} \cdot h_{\text{water}}.
ρliquid=ρwater×hwaterhliquid\rho_{\text{liquid}} = \rho_{\text{water}} \times \frac{h_{\text{water}}}{h_{\text{liquid}}}.
Acceleration due to gravity gg cancels out from both sides of the pressure balance equation.
3
Substitute hliquid=15.0 cmh_{\text{liquid}} = 15.0\text{ cm}, hwater=12.0 cmh_{\text{water}} = 12.0\text{ cm}, and ρwater=1000 kg m3\rho_{\text{water}} = 1000\text{ kg m}^{-3}.
ρliquid=1000×12.015.0=800 kg m3\rho_{\text{liquid}} = 1000 \times \frac{12.0}{15.0} = 800\text{ kg m}^{-3}.
Heights can remain in centimeters since their unit ratio is dimensionless.

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Hydrostatic Pressure Balance in U-Tube Manometers
Tahmini Süre:1m 30s
Soru 956Soru

Element XX exists naturally as three isotopes with mass numbers 2424, 2525, and 2626. The relative atomic mass of element XX is 24.3224.32. If the natural abundance of the isotope 25X^{25}X is 10%10\%, what is the percentage abundance of the isotope 26X^{26}X?

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Cevap: 11

Cevap

The percentage abundance of 26X^{26}X is 11%11\%.
By setting the percentage abundance of 24X^{24}X as xx and 26X^{26}X as zz, given 25X=10%^{25}X = 10\%, we have x+z=90%x + z = 90\%. Using the relative atomic mass formula 24x+25(10)+26z=243224x + 25(10) + 26z = 2432 and substituting x=90zx = 90 - z yields 2410+2z=24322410 + 2z = 2432, solving to z=11%z = 11\%.

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1
Formulate the abundance relation for the three isotopes.
The sum of abundances is x+10+z=100%x + 10 + z = 100\%, which gives x=90zx = 90 - z.
The sum of percentage abundances of all naturally occurring isotopes of an element must equal 100%.
2
Set up the weighted relative atomic mass equation.
24x+25(10)+26z=243224x + 25(10) + 26z = 2432.
Relative atomic mass is the weighted average of isotopic masses based on fractional abundance.
3
Substitute x=90zx = 90 - z and solve for zz.
24(90z)+250+26z=2432    2410+2z=2432    z=11%24(90 - z) + 250 + 26z = 2432 \implies 2410 + 2z = 2432 \implies z = 11\%.
Substituting xx reduces the equation to a single variable zz, representing the percentage abundance of 26X^{26}X.

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Calculation of Isotopic Abundances from Relative Atomic Mass
Soru 957Soru

Element MM has a relative atomic mass of 24.3224.32. It exists naturally as three isotopes: 24M^{24}M with a relative abundance of 79%79\%, 25M^{25}M with a relative abundance of 10%10\%, and an isotope xM^{x}M with a relative abundance of 11%11\%. What is the mass number (xx) of the third isotope?

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Cevap: 26

Cevap

The mass number of the third isotope is 26.
The relative atomic mass is the weighted average of isotopic mass numbers: 24.32=(24×79)+(25×10)+(x×11)10024.32 = \frac{(24 \times 79) + (25 \times 10) + (x \times 11)}{100}. Simplifying gives 2432=1896+250+11x2432 = 1896 + 250 + 11x, which simplifies to 11x=28611x = 286, yielding x=26x = 26.

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1
Set up the relative atomic mass equation based on percentage abundances.
RAM=(24×0.79)+(25×0.10)+(x×0.11)\text{RAM} = (24 \times 0.79) + (25 \times 0.10) + (x \times 0.11)
The relative atomic mass of an element is the weighted average of the mass numbers of its naturally occurring isotopes.
2
Calculate the mass contributions of the first two isotopes.
24×0.79=18.9624 \times 0.79 = 18.96 and 25×0.10=2.5025 \times 0.10 = 2.50, giving a combined sum of 21.4621.46
Evaluating the contribution of known isotopes isolates the variable term.
3
Subtract the combined contribution from the given relative atomic mass to find the contribution of the third isotope.
0.11x=24.3221.46=2.860.11x = 24.32 - 21.46 = 2.86
The remaining mass contribution must come entirely from the third isotope.
4
Divide by the fractional abundance of the third isotope to solve for xx.
x=2.860.11=26x = \frac{2.86}{0.11} = 26
Dividing the mass contribution by fractional abundance yields the integer mass number.

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Relative Atomic Mass Calculation from Isotopic Abundances
Tahmini Süre:1m 15s
Soru 958Soru

A Geiger-Müller counter records a total count rate of 340 counts per minute340\text{ counts per minute} near a radioactive source. The background radiation in the laboratory produces a steady count rate of 20 counts per minute20\text{ counts per minute}. If the total count rate recorded by the counter drops to 60 counts per minute60\text{ counts per minute} after an elapsed time of 15 minutes15\text{ minutes}, what is the half-life of the radioactive source in minutes?

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Cevap: 5

Cevap

The half-life of the radioactive source is 5 minutes5\text{ minutes}.
To find the true activity of the radioactive source, the constant background radiation of 20 cpm20\text{ cpm} must be subtracted from all detector readings. The initial source activity is 34020=320 cpm340 - 20 = 320\text{ cpm} and the activity after 15 minutes15\text{ minutes} is 6020=40 cpm60 - 20 = 40\text{ cpm}. The fraction of source activity remaining is 40/320=1/8=(1/2)340 / 320 = 1/8 = (1/2)^3, which means 33 half-lives have elapsed in 15 minutes15\text{ minutes}. Dividing the total time by the number of half-lives (15/315 / 3) gives a half-life of 5 minutes5\text{ minutes}.

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1
Calculate the initial activity of the radioactive source by subtracting the background count rate.
A0=340 cpm20 cpm=320 cpmA_0 = 340\text{ cpm} - 20\text{ cpm} = 320\text{ cpm}
Background radiation contributes to the detector reading and must be isolated from the source activity.
2
Calculate the activity of the source after 15 minutes by subtracting the background count rate.
A(t)=60 cpm20 cpm=40 cpmA(t) = 60\text{ cpm} - 20\text{ cpm} = 40\text{ cpm}
The background count remains constant at 20 cpm20\text{ cpm}, so the actual count due to the source is 40 cpm40\text{ cpm}.
3
Determine the remaining fraction of the radioactive source.
A(t)A0=40320=18\frac{A(t)}{A_0} = \frac{40}{320} = \frac{1}{8}
Radioactive decay follows an exponential decay law based on the fraction of initial undecayed nuclei.
4
Calculate the number of elapsed half-lives nn.
\left(\frac{1}{2}\right)^n = \frac{1}{8} = \left(\frac{1}{2}\right)^3 \implies n = 3
The remaining fraction equals (1/2)n(1/2)^n where nn is the number of half-lives.
5
Compute the half-life T1/2T_{1/2}.
T_{1/2} = \frac{t}{n} = \frac{15\text{ minutes}}{3} = 5\text{ minutes}
The total elapsed time is the product of the number of half-lives and the duration of one half-life.

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Radioactive Decay Law and Half-life with Background Radiation Correction
Soru 959Soru

A sample of a radioactive substance has a decay constant of 0.0154 h10.0154\text{ h}^{-1}. What is the elapsed time, in hours, required for 87.5%87.5\% of the original sample to decay? (Take ln2=0.693\ln 2 = 0.693)

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Cevap: 135

Cevap

135 hours
First, calculate the half-life of the substance using the relation T1/2=ln2λ=0.6930.0154 h1=45 hoursT_{1/2} = \frac{\ln 2}{\lambda} = \frac{0.693}{0.0154\text{ h}^{-1}} = 45\text{ hours}. Since 87.5%87.5\% of the sample has decayed, the remaining fraction of the sample is 100%87.5%=12.5%=18100\% - 87.5\% = 12.5\% = \frac{1}{8}. Expressing 18\frac{1}{8} as a power of 12\frac{1}{2} gives (12)3\left(\frac{1}{2}\right)^3, indicating that 33 half-lives have passed. The total elapsed time is therefore 3×45 hours=135 hours3 \times 45\text{ hours} = 135\text{ hours}.

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1
Calculate the half-life from the given decay constant
Half-life T1/2=45 hoursT_{1/2} = 45\text{ hours}
The decay constant λ\lambda and half-life T1/2T_{1/2} are related by the formula T1/2=ln2λT_{1/2} = \frac{\ln 2}{\lambda}
2
Find the remaining percentage and fraction of the sample
Remaining fraction is 12.5%12.5\% or 18\frac{1}{8}
Radioactive decay equations use the undecayed remaining amount, which is 100%87.5%=12.5%100\% - 87.5\% = 12.5\%
3
Calculate the number of half-lives elapsed
Number of half-lives n=3n = 3
Since (12)n=18\left(\frac{1}{2}\right)^n = \frac{1}{8}, solving for nn gives n=3n = 3
4
Compute the total elapsed time
Total elapsed time t=135 hourst = 135\text{ hours}
Total elapsed time is the product of the number of half-lives and the half-life duration (3×45 hours3 \times 45\text{ hours})

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Radioactive Decay Law and Half-life Relationship
Soru 960Soru

A uniform beam PQPQ of length 4.0 m4.0\text{ m} and mass 20 kg20\text{ kg} is supported horizontally on a pivot at end PP and by a vertical wire attached at end QQ. A load of mass 30 kg30\text{ kg} is placed on the beam at a distance of 1.0 m1.0\text{ m} from PP. Taking the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the tension in the vertical wire attached at QQ in newtons?

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Cevap: 175

Cevap

The tension in the vertical wire attached at end QQ is 175 N175\text{ N}.
By applying the principle of moments about the pivot at PP, the sum of downward clockwise moments produced by the 30 kg30\text{ kg} load (300 N×1.0 m=300 Nm300\text{ N} \times 1.0\text{ m} = 300\text{ N}\cdot\text{m}) and the beam's center of gravity (200 N×2.0 m=400 Nm200\text{ N} \times 2.0\text{ m} = 400\text{ N}\cdot\text{m}) equals 700 Nm700\text{ N}\cdot\text{m}. Equating this to the counterclockwise moment of the tension force (T×4.0 mT \times 4.0\text{ m}) gives T=175 NT = 175\text{ N}.

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1
Determine forces and their perpendicular distances from the pivot at PP.
The load exerts a downward force of 300 N300\text{ N} at 1.0 m1.0\text{ m} from PP. The uniform beam's weight of 200 N200\text{ N} acts at its midpoint (2.0 m2.0\text{ m} from PP). The vertical tension TT acts upward at QQ (4.0 m4.0\text{ m} from PP).
Before applying the principle of moments, all force magnitudes and their distance arms relative to the pivot point must be identified.
2
Equate total clockwise moments to total counterclockwise moments about PP.
(300 N×1.0 m)+(200 N×2.0 m)=T×4.0 m(300\text{ N} \times 1.0\text{ m}) + (200\text{ N} \times 2.0\text{ m}) = T \times 4.0\text{ m}
For rotational equilibrium, the sum of clockwise moments about any pivot must equal the sum of counterclockwise moments about that same pivot.
3
Calculate the value of the tension force TT.
T=7004.0=175 NT = \frac{700}{4.0} = 175\text{ N}
Simplifying the moment equation gives the magnitude of the upward supporting force.

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Principle of Moments and Rotational Equilibrium
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