Tüm alıştırma soruları

1526 soru

Soru 1461Soru

A consumer obtains a total utility (TUTU) of 1818 utils, 3232 utils, 4242 utils, 4848 utils, and 5050 utils from consuming 11, 22, 33, 44, and 55 cups of coffee, respectively. What is the marginal utility (MUMU) derived from consuming the 4th4^{\text{th}} cup of coffee?

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Cevap: 6

Cevap

The marginal utility derived from consuming the 4th cup of coffee is 6 utils.
Marginal Utility (MUMU) represents the extra utility gained from consuming an additional unit of a commodity. It is computed as MU=TUnTUn1MU = TU_n - TU_{n-1}. For the 4th cup of coffee, MU4=TU4TU3=4842=6MU_4 = TU_4 - TU_3 = 48 - 42 = 6 utils.

Adım Adım Çözüm

1
Identify the Total Utility for the target unit and the preceding unit
TU4=48TU_4 = 48 utils and TU3=42TU_3 = 42 utils
Marginal Utility measures the addition to total utility from consuming one more unit.
2
Apply the Marginal Utility formula MU=ΔTUΔQMU = \frac{\Delta TU}{\Delta Q}
MU4=484243=61=6MU_4 = \frac{48 - 42}{4 - 3} = \frac{6}{1} = 6 utils
The change in quantity is 1 unit, so MUMU is simply the difference between TU4TU_4 and TU3TU_3.

Anahtar Kavram

Calculation of Marginal Utility from Total Utility schedule
Tahmini Süre:1m 0s
Soru 1462Soru

A particle of mass 0.20 kg0.20\text{ kg} executes simple harmonic motion with an amplitude of 0.05 m0.05\text{ m} and a period of oscillation of 0.20π s0.20\pi\text{ s}. What is the maximum kinetic energy of the particle in joules?

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Cevap: 0.025

Cevap

The maximum kinetic energy of the particle is 0.025 J0.025\text{ J}.
The maximum kinetic energy occurs at the equilibrium position where speed reaches its maximum value vmax=ωAv_{\text{max}} = \omega A. Substituting ω=2π0.20π=10 rad/s\omega = \frac{2\pi}{0.20\pi} = 10\text{ rad/s} into the maximum speed formula gives vmax=10×0.05=0.50 m/sv_{\text{max}} = 10 \times 0.05 = 0.50\text{ m/s}. Computing kinetic energy yields Ek=12(0.20)(0.50)2=0.025 JE_k = \frac{1}{2} (0.20) (0.50)^2 = 0.025\text{ J}.

Adım Adım Çözüm

1
Calculateangularfrequency(ω)Calculate angular frequency (\omega)
ω=10 rad/s\omega = 10\text{ rad/s}
Using the relation ω=2πT\omega = \frac{2\pi}{T} with T=0.20π sT = 0.20\pi\text{ s}.
2
Calculate maximum speed (v_{max})
v_{max} = 0.50\text{ m/s}
Maximum velocity occurs at the equilibrium position and is given by vmax=ωAv_{\text{max}} = \omega A.
3
Calculate maximum kinetic energy (E_k)
E_k = 0.025\text{ J}
Using the kinetic energy formula Ek=12mv2E_k = \frac{1}{2} m v^2 at maximum velocity.

Anahtar Kavram

Energy conservation and maximum speed in Simple Harmonic Motion
Soru 1463Soru

A poultry farm operates in a perfectly competitive market where the market price per crate of eggs is N70\text{N}70. The farm's short-run total cost function is TC=2Q2+10Q+200TC = 2Q^2 + 10Q + 200, where QQ is the quantity of crates produced and TCTC is the total cost in Naira. What is the maximum economic profit, in Naira, realized by the farm?

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Cevap: 250

Cevap

The maximum economic profit realized by the farm is 250 Naira.
In a perfectly competitive market, the firm is a price taker so marginal revenue equals market price (MR=P=70MR = P = 70). Equating marginal revenue to marginal cost (MC=4Q+10MC = 4Q + 10) gives an equilibrium output of Q=15Q = 15 units. Substituting Q=15Q = 15 into Total Revenue (TR=70×15=1050TR = 70 \times 15 = 1050) and Total Cost (TC=2(15)2+10(15)+200=800TC = 2(15)^2 + 10(15) + 200 = 800) yields an economic profit of 1050800=N2501050 - 800 = \text{N}250.

Adım Adım Çözüm

1
Derive the Marginal Cost equation from Total Cost
MC=4Q+10MC = 4Q + 10
Marginal Cost represents the rate of change of Total Cost with respect to output.
2
Equate Marginal Revenue (which equals price in perfect competition) to Marginal Cost
70=4Q+10    Q=1570 = 4Q + 10 \implies Q = 15 units
A price-taking firm maximizes profit where price equals marginal cost (P=MCP = MC).
3
Calculate Total Revenue at optimal output level
TR=70×15=N1050TR = 70 \times 15 = \text{N}1050
Total revenue is the product of price per unit and total output sold.
4
Calculate Total Cost at optimal output level
TC=2(15)2+10(15)+200=N800TC = 2(15)^2 + 10(15) + 200 = \text{N}800
Substitute optimal output into the total cost function.
5
Subtract Total Cost from Total Revenue to find economic profit
Profit=1050800=N250\text{Profit} = 1050 - 800 = \text{N}250
Economic profit is the surplus remaining after deducting total explicit and fixed cost from total revenue.

Anahtar Kavram

Profit Maximization in Perfect Competition
Tahmini Süre:1m 30s
Soru 1464Soru

A spherical black body radiator with an initial radius of 0.10 m0.10\text{ m} emits thermal radiation at a rate of E1E_1 when its surface temperature is 400 K400\text{ K}. If the radius of the sphere is doubled to 0.20 m0.20\text{ m} and its absolute temperature is reduced to 200 K200\text{ K}, what is the value of the ratio of the new rate of heat radiation to the initial rate, E2E1\frac{E_2}{E_1}?

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Cevap: 0.25

Cevap

The ratio of the new rate of heat radiation to the initial rate is 0.250.25.
According to the Stefan-Boltzmann law, the rate of thermal radiation emitted by a black body is directly proportional to its surface area (Ar2A \propto r^2) and the fourth power of its absolute temperature (T4T^4). Doubling the radius increases the surface area by a factor of 22=42^2 = 4, while halving the absolute temperature decreases the radiation rate per unit area by a factor of (1/2)4=1/16(1/2)^4 = 1/16. The net ratio of the new emission rate to the initial emission rate is 4×(1/16)=0.254 \times (1/16) = 0.25.

Adım Adım Çözüm

1
Apply Stefan-Boltzmann's law of radiation to formulate the rate of heat emission.
The total power radiated by a sphere of radius rr at thermodynamic temperature TT is given by P=σAT4=4πσr2T4P = \sigma A T^4 = 4\pi \sigma r^2 T^4, where σ\sigma is the Stefan-Boltzmann constant.
Thermal radiation emission rate depends directly on surface area (A=4πr2A = 4\pi r^2) and the fourth power of absolute temperature (T4T^4).
2
Formulate the ratio E2E1\frac{E_2}{E_1} using the scaled physical parameters.
E2E1=4πσr22T244πσr12T14=(r2r1)2(T2T1)4\frac{E_2}{E_1} = \frac{4\pi \sigma r_2^2 T_2^4}{4\pi \sigma r_1^2 T_1^4} = \left(\frac{r_2}{r_1}\right)^2 \left(\frac{T_2}{T_1}\right)^4
Constants 4πσ4\pi\sigma cancel out when evaluating relative changes.
3
Substitute the given numerical ratios into the equation and compute the result.
Given r2r1=0.200.10=2\frac{r_2}{r_1} = \frac{0.20}{0.10} = 2 and T2T1=200400=0.5\frac{T_2}{T_1} = \frac{200}{400} = 0.5, we get E2E1=(2)2×(0.5)4=4×116=0.25\frac{E_2}{E_1} = (2)^2 \times (0.5)^4 = 4 \times \frac{1}{16} = 0.25.
Evaluating 22=42^2 = 4 and (0.5)4=1/16(0.5)^4 = 1/16 yields a final ratio of 4/16=0.254/16 = 0.25.

Anahtar Kavram

Stefan-Boltzmann Law of Radiation
Soru 1465Soru

A light ray strikes a plane mirror. Keeping the direction of the incident ray fixed, the mirror is rotated through an angle of 1515^\circ about an axis lying in its plane. What is the angle of rotation, in degrees, of the reflected ray?

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Cevap: 30

Cevap

The reflected ray turns through an angle of 3030^\circ.
When a plane mirror is rotated through an angle θ\theta while keeping the incident ray direction constant, the normal turns by θ\theta. This changes the angle of incidence by θ\theta and the angle of reflection by θ\theta, causing the reflected ray to rotate by a total angle of 2θ2\theta. For a mirror rotation of 1515^\circ, the reflected ray rotates through 2×15=302 \times 15^\circ = 30^\circ.

Adım Adım Çözüm

1
Analyze the effect of mirror rotation on the normal line
When the plane mirror rotates by 1515^\circ, the normal to the mirror surface also rotates by 1515^\circ.
The normal line is always perpendicular to the surface of the mirror.
2
Determine the change in the angle of incidence and reflection
The angle of incidence changes by 1515^\circ, so the angle of reflection relative to the new normal also changes by 1515^\circ.
According to the law of reflection, the angle of incidence equals the angle of reflection (i=ri = r).
3
Calculate the total angular deviation of the reflected ray
The total shift of the reflected ray relative to its original path is 15+15=3015^\circ + 15^\circ = 30^\circ.
The rotation of the reflected ray is twice the angle of rotation of the mirror.

Anahtar Kavram

Rotation of Reflected Ray by a Plane Mirror
Soru 1466Soru

A glass prism with a refracting angle of 6060^\circ has a refractive index of 2\sqrt{2}. What is the angle of minimum deviation, in degrees, experienced by a light ray passing through this prism?

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Cevap: 30

Cevap

The angle of minimum deviation is 3030^\circ.
Using the prism minimum deviation relation n=sin((A+Dm)/2)sin(A/2)n = \frac{\sin\left((A + D_m)/2\right)}{\sin(A/2)}, substituting n=2n = \sqrt{2} and A=60A = 60^\circ yields sin((60+Dm)/2)=12\sin\left((60^\circ + D_m)/2\right) = \frac{1}{\sqrt{2}}. This gives (60+Dm)/2=45(60^\circ + D_m)/2 = 45^\circ, so Dm=30D_m = 30^\circ.

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1
Apply the prism minimum deviation equation.
n=sin(A+Dm2)sin(A2)n = \frac{\sin\left(\frac{A + D_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}
This relates refractive index, prism refracting angle, and minimum deviation angle.
2
Substitute the given values A=60A = 60^\circ and n=2n = \sqrt{2}.
2=sin(60+Dm2)sin(30)\sqrt{2} = \frac{\sin\left(\frac{60^\circ + D_m}{2}\right)}{\sin(30^\circ)}
Dividing the refracting angle 6060^\circ by 2 gives 3030^\circ for the denominator angle.
3
Calculate the numerator sine term.
sin(60+Dm2)=12\sin\left(\frac{60^\circ + D_m}{2}\right) = \frac{1}{\sqrt{2}}
Multiplying 2\sqrt{2} by sin(30)=0.5\sin(30^\circ) = 0.5 gives 22=12\frac{\sqrt{2}}{2} = \frac{1}{\sqrt{2}}.
4
Solve for the angle DmD_m.
Dm=30D_m = 30^\circ
Since arcsin(12)=45\arcsin\left(\frac{1}{\sqrt{2}}\right) = 45^\circ, we have 60+Dm2=45\frac{60^\circ + D_m}{2} = 45^\circ, leading to 60+Dm=9060^\circ + D_m = 90^\circ.

Anahtar Kavram

Minimum Deviation in Triangular Prisms
Soru 1467Soru

A block of transparent polymer with a refractive index of 1.251.25 is placed over a small mark on a table. When viewed vertically from directly above, the mark appears to be shifted upward by 3.0 cm3.0\text{ cm}. What is the real thickness of the polymer block in centimeters?

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Cevap: 15

Cevap

The real thickness of the polymer block is 15.0 cm15.0\text{ cm}.
Refraction at the interface produces an upward shift s=d(11n)s = d\left(1 - \frac{1}{n}\right). Substituting s=3.0 cms = 3.0\text{ cm} and n=1.25n = 1.25 gives 3.0=d(10.80)=0.20d3.0 = d(1 - 0.80) = 0.20d, which solves to a real thickness d=15.0 cmd = 15.0\text{ cm}.

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1
Relate apparent depth dd' to real depth dd using the refractive index.
d=dnd' = \frac{d}{n}
Light refracting at the surface of a denser medium causes the object to appear at a shallower depth.
2
Express the apparent displacement (upward shift) ss in terms of dd and nn.
s=dd=d(11n)s = d - d' = d\left(1 - \frac{1}{n}\right)
The upward shift is the vertical distance between the true position and the apparent position.
3
Substitute s=3.0 cms = 3.0\text{ cm} and n=1.25n = 1.25 into the equation and solve for dd.
3.0=d(111.25)=d(10.80)=0.20d    d=15.0 cm3.0 = d\left(1 - \frac{1}{1.25}\right) = d(1 - 0.80) = 0.20 d \implies d = 15.0\text{ cm}
Algebraic evaluation yields the exact real thickness of the polymer block.

Anahtar Kavram

Apparent depth and upward displacement due to refraction
Soru 1468Soru

A crate of mass 5 kg5\text{ kg} is pulled from rest along a smooth inclined plane tilted at 3030^\circ to the horizontal by a constant force of 40 N40\text{ N} acting parallel to the slope. What is the kinetic energy of the crate in Joules after moving a distance of 6 m6\text{ m} along the incline? (Take g=10 m s2g = 10\text{ m s}^{-2})

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Cevap: 90

Cevap

The final kinetic energy of the crate is 90 J90\text{ J}.
The kinetic energy gained equals the net work done on the crate. The total work put in by the pulling force is 40×6=240 J40 \times 6 = 240\text{ J}, while the gravitational potential energy gained is 5×10×(6sin30)=150 J5 \times 10 \times (6 \sin 30^\circ) = 150\text{ J}. Subtracting the potential energy gained from the total work gives a net kinetic energy of 240150=90 J240 - 150 = 90\text{ J}.

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1
Calculate the total work done by the applied force parallel to the incline
Wapplied=40 N×6 m=240 JW_{\text{applied}} = 40\text{ N} \times 6\text{ m} = 240\text{ J}
Work done by a force is equal to force multiplied by displacement in the direction of the force.
2
Calculate the work done against gravity (potential energy gained)
ΔPE=mgdsin(30)=5×10×6×0.5=150 J\Delta PE = m g d \sin(30^\circ) = 5 \times 10 \times 6 \times 0.5 = 150\text{ J}
The height gained along an incline of length dd and angle θ\theta is h=dsinθh = d \sin\theta.
3
Determine the net work done to find the final kinetic energy
KE=WappliedΔPE=240 J150 J=90 JKE = W_{\text{applied}} - \Delta PE = 240\text{ J} - 150\text{ J} = 90\text{ J}
According to the work-energy theorem, the net work done on an object equals its change in kinetic energy.

Anahtar Kavram

Work-Energy Theorem on an Inclined Plane
Soru 1469Soru

A body of mass 0.40 kg0.40\text{ kg} is attached to a light helical spring and set into simple harmonic motion. If the system oscillates with a period of 0.40π s0.40\pi\text{ s}, what is the force constant of the spring in N/m\text{N/m}?

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Cevap: 10

Cevap

The force constant of the spring is 10 N/m10\text{ N/m}.
The period of a mass-spring system undergoing simple harmonic motion is given by T=2πmkT = 2\pi \sqrt{\frac{m}{k}}. Substituting m=0.40 kgm = 0.40\text{ kg} and T=0.40π sT = 0.40\pi\text{ s} yields 0.40π=2π0.40k0.40\pi = 2\pi \sqrt{\frac{0.40}{k}}. Dividing both sides by 2π2\pi gives 0.20=0.40k0.20 = \sqrt{\frac{0.40}{k}}. Squaring both sides yields 0.04=0.40k0.04 = \frac{0.40}{k}, which gives k=10 N/mk = 10\text{ N/m}.

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1
Identify the period relationship for a spring-mass SHM system
T=2πmkT = 2\pi \sqrt{\frac{m}{k}}
This formula relates the period of oscillation TT to the mass mm and spring constant kk.
2
Substitute the given mass and period into the equation
0.40π=2π0.40k0.40\pi = 2\pi \sqrt{\frac{0.40}{k}}
Given that m=0.40 kgm = 0.40\text{ kg} and T=0.40π sT = 0.40\pi\text{ s}.
3
Simplify the equation by isolating the square root term
0.40k=0.20\sqrt{\frac{0.40}{k}} = 0.20
Dividing both sides of the equation by 2π2\pi isolates the radical.
4
Square both sides and solve for the spring constant kk
k=10 N/mk = 10\text{ N/m}
Squaring yields 0.04=0.40k0.04 = \frac{0.40}{k}, which rearranges to k=0.400.04=10 N/mk = \frac{0.40}{0.04} = 10\text{ N/m}.

Anahtar Kavram

Period of oscillation of a mass-spring system in Simple Harmonic Motion
Tahmini Süre:1m 30s
Soru 1470Soru

At a certain research station, the vertical component of the Earth's magnetic field is measured as 2.4×105 T2.4 \times 10^{-5}\text{ T}. If the angle of dip at this station is 3737^\circ (given sin37=0.60\sin 37^\circ = 0.60 and cos37=0.80\cos 37^\circ = 0.80), calculate the horizontal component of the Earth's magnetic field in μT\mu\text{T}.

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Cevap: 32

Cevap

The horizontal component of the Earth's magnetic field is 32 μT32\ \mu\text{T}.
The horizontal component BhB_h and vertical component BvB_v of the Earth's magnetic field are related by tanθ=BvBh\tan \theta = \frac{B_v}{B_h}, where θ\theta is the angle of dip. Given Bv=2.4×105 T=24 μTB_v = 2.4 \times 10^{-5}\text{ T} = 24\ \mu\text{T} and tan37=0.75\tan 37^\circ = 0.75, rearranging gives Bh=240.75=32 μTB_h = \frac{24}{0.75} = 32\ \mu\text{T}.

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1
Express the relationship between the vertical component (BvB_v), horizontal component (BhB_h), and angle of dip (θ\theta).
tanθ=BvBh\tan \theta = \frac{B_v}{B_h}
By definition of the angle of dip in the magnetic meridian, the tangent of the dip angle equals the ratio of the vertical component to the horizontal component.
2
Calculate tan37\tan 37^\circ using the provided trigonometric values.
tan37=0.600.80=0.75\tan 37^\circ = \frac{0.60}{0.80} = 0.75
Tangent of an angle is the ratio of sine to cosine of that angle.
3
Convert BvB_v from teslas to microteslas.
Bv=2.4×105 T=24 μTB_v = 2.4 \times 10^{-5}\text{ T} = 24\ \mu\text{T}
Since 1 μT=106 T1\ \mu\text{T} = 10^{-6}\text{ T}, 2.4×105 T=24×106 T=24 μT2.4 \times 10^{-5}\text{ T} = 24 \times 10^{-6}\text{ T} = 24\ \mu\text{T}.
4
Rearrange the equation to solve for BhB_h and substitute the values.
Bh=Bvtanθ=24 μT0.75=32 μTB_h = \frac{B_v}{\tan \theta} = \frac{24\ \mu\text{T}}{0.75} = 32\ \mu\text{T}
Dividing 2424 by 0.750.75 yields 3232.

Anahtar Kavram

Resolution of Earth's magnetic field into horizontal and vertical components
Soru 1471Soru

An alternating current (AC) circuit consists of a resistor of resistance R=30 ΩR = 30\ \Omega, an inductor of inductive reactance XL=80 ΩX_L = 80\ \Omega, and a capacitor of capacitive reactance XC=40 ΩX_C = 40\ \Omega connected in series across an AC source of RMS voltage 150 V150\ \text{V}. What is the average power dissipated in the circuit in watts?

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Cevap: 270

Cevap

The average power dissipated in the circuit is 270 W270\ \text{W}.
The total impedance of a series RLC circuit is Z=R2+(XLXC)2=302+(8040)2=50 ΩZ = \sqrt{R^2 + (X_L - X_C)^2} = \sqrt{30^2 + (80 - 40)^2} = 50\ \Omega. The RMS current is Irms=VrmsZ=15050=3 AI_{\text{rms}} = \frac{V_{\text{rms}}}{Z} = \frac{150}{50} = 3\ \text{A}. Because pure inductors and capacitors consume zero average power over a complete cycle, power is dissipated only across the resistor, giving P=Irms2R=32×30=270 WP = I_{\text{rms}}^2 R = 3^2 \times 30 = 270\ \text{W}.

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1
Calculate net reactance
X=40 ΩX = 40\ \Omega
Inductive and capacitive reactances oppose each other in phase, so net reactance is XLXCX_L - X_C.
2
Calculate total circuit impedance
Z=50 ΩZ = 50\ \Omega
Resistance and net reactance add in quadrature: Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}.
3
Calculate RMS current
Irms=3 AI_{\text{rms}} = 3\ \text{A}
Ohm's law for AC circuits gives Irms=VrmsZI_{\text{rms}} = \frac{V_{\text{rms}}}{Z}.
4
Calculate average power dissipated
P=270 WP = 270\ \text{W}
Power is dissipated exclusively by resistance in an AC circuit: P=Irms2RP = I_{\text{rms}}^2 R.

Anahtar Kavram

Power Dissipation in AC Circuits
Tahmini Süre:1m 30s
Soru 1472Soru

A container holds a layer of water of depth 16.0 cm16.0\text{ cm}. An immiscible layer of oil of refractive index 1.201.20 and thickness 6.0 cm6.0\text{ cm} floats on top of the water. If the refractive index of water is 1.331.33 (or 43\frac{4}{3}), what is the total apparent depth, in centimeters, of a small object resting at the bottom of the container when viewed normally from directly above?

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Cevap: 17

Cevap

The total apparent depth of the object when viewed normally from directly above is 17.0 cm17.0\text{ cm}.
When an object at the bottom of a container is viewed normally through multiple transparent media, the overall apparent depth is the sum of the apparent depths produced by each medium individually (dapp=dinid_{\text{app}} = \sum \frac{d_i}{n_i}). Substituting the given values gives 16.04/3+6.01.20=12.0 cm+5.0 cm=17.0 cm\frac{16.0}{4/3} + \frac{6.0}{1.20} = 12.0\text{ cm} + 5.0\text{ cm} = 17.0\text{ cm}.

Adım Adım Çözüm

1
Calculate the apparent depth of the water layer.
Apparent depth of water = 12.0 cm12.0\text{ cm}
Apparent depth in a single medium is given by the real depth divided by its refractive index (dapp=d/nd_{\text{app}} = d / n). For water, 16.04/3=12.0 cm\frac{16.0}{4/3} = 12.0\text{ cm}.
2
Calculate the apparent depth of the oil layer.
Apparent depth of oil = 5.0 cm5.0\text{ cm}
Using dapp=d/nd_{\text{app}} = d / n for the oil layer, 6.01.20=5.0 cm\frac{6.0}{1.20} = 5.0\text{ cm}.
3
Sum the apparent depths of both media.
Total apparent depth = 17.0 cm17.0\text{ cm}
For multiple parallel transparent layers, the total apparent depth is the sum of the apparent depths of each individual layer.

Anahtar Kavram

Apparent depth in composite media layers
Soru 1473Soru

The saturated vapour pressure of water in an enclosed space is 25 mmHg25\text{ mmHg}. If the relative humidity within the space is measured to be 64%64\%, what is the partial pressure of the water vapour in mmHg\text{mmHg}?

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Cevap: 16

Cevap

The partial pressure of the water vapour in the enclosed space is 16 mmHg16\text{ mmHg}.
Relative humidity is defined as the ratio of the actual partial pressure of water vapour present in a given volume of air to the saturated vapour pressure at the same temperature, expressed as a percentage: R.H.=PS.V.P.×100%\text{R.H.} = \frac{P}{\text{S.V.P.}} \times 100\%. Rearranging this equation gives P=R.H.×S.V.P.100=64×25100=16 mmHgP = \frac{\text{R.H.} \times \text{S.V.P.}}{100} = \frac{64 \times 25}{100} = 16\text{ mmHg}.

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1
Identify the given parameters and state the relative humidity formula.
Relative Humidity (R.H.) = 64%64\%, Saturated Vapour Pressure (S.V.P.) = 25 mmHg25\text{ mmHg}. R.H.=PS.V.P.×100%\text{R.H.} = \frac{P}{\text{S.V.P.}} \times 100\%.
Relative humidity relates the actual partial vapour pressure present to the maximum saturated vapour pressure possible at that temperature.
2
Substitute the values into the equation and solve for partial pressure PP.
64=P25×100    64=4P    P=16 mmHg64 = \frac{P}{25} \times 100 \implies 64 = 4P \implies P = 16\text{ mmHg}.
Dividing 100100 by 2525 yields a factor of 44, allowing clean mental computation.

Anahtar Kavram

Relationship between relative humidity, partial vapour pressure, and saturated vapour pressure.
Soru 1474Soru

An electric heater rated at 200 W200\text{ W} is used to heat a liquid of mass 1.5 kg1.5\text{ kg} for 7 minutes7\text{ minutes}. If the temperature of the liquid rises from 25C25^\circ\text{C} to 65C65^\circ\text{C}, assuming no heat energy is lost to the surroundings, what is the specific heat capacity of the liquid in Jkg1K1\text{J}\text{kg}^{-1}\text{K}^{-1}?

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Cevap: 1400

Cevap

The specific heat capacity of the liquid is 1400 Jkg1K11400\text{ J}\text{kg}^{-1}\text{K}^{-1}.
The electrical energy supplied over 7 minutes7\text{ minutes} (420 s420\text{ s}) at a power rating of 200 W200\text{ W} equals 84,000 J84,000\text{ J}. Equating this total energy to thermal absorption Q=mcΔTQ = m c \Delta T for a 1.5 kg1.5\text{ kg} mass experiencing a 40 K40\text{ K} temperature rise gives c=84,0001.5×40=1400 Jkg1K1c = \frac{84,000}{1.5 \times 40} = 1400\text{ J}\text{kg}^{-1}\text{K}^{-1}.

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1
Convert heating time to seconds and compute total heat energy supplied.
t=7×60=420 st = 7 \times 60 = 420\text{ s}, so Q=P×t=200×420=84,000 JQ = P \times t = 200 \times 420 = 84,000\text{ J}.
Electrical power is the rate of energy transfer (P=Q/tP = Q/t), so heat energy equals power multiplied by time in seconds.
2
Calculate temperature difference.
ΔT=65C25C=40 K\Delta T = 65^\circ\text{C} - 25^\circ\text{C} = 40\text{ K}.
The temperature rise drives heat absorption according to the thermal equation.
3
Rearrange the heat energy formula Q=mcΔTQ = m c \Delta T to find the specific heat capacity cc.
c=84,0001.5×40=84,00060=1400 Jkg1K1c = \frac{84,000}{1.5 \times 40} = \frac{84,000}{60} = 1400\text{ J}\text{kg}^{-1}\text{K}^{-1}.
Specific heat capacity represents the heat energy required per unit mass per unit temperature change.

Anahtar Kavram

Specific heat capacity calculation using electrical energy input (Q=Pt=mcΔTQ = P t = m c \Delta T).
Tahmini Süre:1m 15s
Soru 1475Soru

A particle executes simple harmonic motion with an amplitude of 0.10 m0.10\text{ m}. At what displacement from its equilibrium position, in meters, is the kinetic energy of the particle equal to three times its potential energy?

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Cevap: 0.05

Cevap

The displacement from the equilibrium position is 0.05 m0.05\text{ m}.
In simple harmonic motion, potential energy is Ep=12kx2E_p = \frac{1}{2}kx^2 and kinetic energy is Ek=12k(A2x2)E_k = \frac{1}{2}k(A^2 - x^2). Setting Ek=3EpE_k = 3E_p gives A2x2=3x2A^2 - x^2 = 3x^2, which simplifies to A2=4x2A^2 = 4x^2, or x=A2x = \frac{A}{2}. Given an amplitude A=0.10 mA = 0.10\text{ m}, the displacement is x=0.10 m2=0.05 mx = \frac{0.10\text{ m}}{2} = 0.05\text{ m}.

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1
Set up the relation between kinetic energy and potential energy using the given condition.
Ek=3Ep    12k(A2x2)=3(12kx2)E_k = 3E_p \implies \frac{1}{2}k(A^2 - x^2) = 3\left(\frac{1}{2}kx^2\right)
In simple harmonic motion, energy is partitioned between kinetic and potential forms based on displacement xx.
2
Solve the algebraic equation for displacement xx in terms of amplitude AA.
A2x2=3x2    A2=4x2    x=A2A^2 - x^2 = 3x^2 \implies A^2 = 4x^2 \implies x = \frac{A}{2}
Canceling the common factor 12k\frac{1}{2}k isolates the geometric parameters AA and xx.
3
Substitute the known amplitude value into the expression for xx.
x=0.10 m2=0.05 mx = \frac{0.10\text{ m}}{2} = 0.05\text{ m}
Plugging in A=0.10 mA = 0.10\text{ m} yields the required displacement.

Anahtar Kavram

Energy Conservation in Simple Harmonic Motion
Soru 1476Soru

The central bank of a country provides the following monetary statistics for a given financial period:

- Currency in circulation outside commercial banks: N420 billion\text{N}420\text{ billion}
- Demand deposits with commercial banks: N980 billion\text{N}980\text{ billion}
- Vault cash held by commercial banks: N90 billion\text{N}90\text{ billion}
- Savings deposits: N650 billion\text{N}650\text{ billion}
- Time deposits: N350 billion\text{N}350\text{ billion}

Based on these data, what is the total broad money supply (M2M_2) in this economy in billions of Naira?

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Cevap: 2400

Cevap

The total broad money supply (M2M_2) in the economy is 2,400 billion Naira2,400\text{ billion Naira}.
Broad money supply (M2M_2) includes narrow money (M1M_1) plus quasi-money (savings deposits and time deposits). M1M_1 is calculated as currency outside banks (420 billion Naira420\text{ billion Naira}) plus demand deposits (980 billion Naira980\text{ billion Naira}), totaling 1,400 billion Naira1,400\text{ billion Naira}. Adding savings deposits (650 billion Naira650\text{ billion Naira}) and time deposits (350 billion Naira350\text{ billion Naira}) yields M2=1,400+650+350=2,400 billion NairaM_2 = 1,400 + 650 + 350 = 2,400\text{ billion Naira}. Commercial bank vault cash is excluded as it is an internal reserve not available in active public circulation.

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1
Calculate Narrow Money (M1M_1)
M1 = 420 + 980 = 1,400 billion Naira
M1 consists of currency in circulation outside commercial banks and demand deposits. Vault cash is excluded as it is not held by the non-bank public.
2
Calculate Quasi-Money (Near Money)
Quasi-Money = 650 + 350 = 1,000 billion Naira
Quasi-money consists of financial assets that are liquid but not directly usable as a medium of exchange, specifically savings deposits and time deposits.
3
Calculate Broad Money (M2M_2)
M2 = 1,400 + 1,000 = 2,400 billion Naira
Broad money supply combines M1 with quasi-money.

Anahtar Kavram

Broad Money Supply (M2) Calculation
Tahmini Süre:1m 30s
Soru 1477Soru

A solid metal component of mass 0.6 kg0.6\text{ kg} absorbs 5400 J5400\text{ J} of thermal energy when its temperature increases from 30C30^\circ\text{C} to 75C75^\circ\text{C}. Calculate the heat capacity of the component in J K1\text{J K}^{-1}.

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Cevap: 120

Cevap

The heat capacity of the metal component is 120 J K1120\text{ J K}^{-1}.
Heat capacity (CC) is calculated by dividing the total thermal energy absorbed (Q=5400 JQ = 5400\text{ J}) by the resulting temperature change (ΔT=75C30C=45 K\Delta T = 75^\circ\text{C} - 30^\circ\text{C} = 45\text{ K}). Performing the division yields C=540045=120 J K1C = \frac{5400}{45} = 120\text{ J K}^{-1}. Note that the mass (0.6 kg0.6\text{ kg}) is not included in the denominator because heat capacity refers to the entire object, unlike specific heat capacity.

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1
Determine the change in temperature
ΔT=75C30C=45 K\Delta T = 75^\circ\text{C} - 30^\circ\text{C} = 45\text{ K}
Heat capacity depends on the temperature difference through which heat energy is absorbed.
2
Apply the definition of heat capacity
C=QΔTC = \frac{Q}{\Delta T}
Heat capacity (CC) is defined as the thermal energy required to raise the temperature of the entire body by 1 K1\text{ K} (or 1C1^\circ\text{C}).
3
Substitute the given thermal energy and temperature change
C=5400 J45 K=120 J K1C = \frac{5400\text{ J}}{45\text{ K}} = 120\text{ J K}^{-1}
Dividing total energy by total temperature rise gives heat capacity.

Anahtar Kavram

Heat capacity (CC) represents the thermal energy needed to change a body's temperature by one unit (C=Q/ΔTC = Q / \Delta T), whereas specific heat capacity (cc) is heat capacity per unit mass (c=C/mc = C / m).
Soru 1478Soru

A planet has a mass equal to 88 times the mass of the Earth and a radius equal to 22 times the radius of the Earth. If the acceleration due to gravity on the surface of the Earth is 10 m/s210\text{ m/s}^2, what is the acceleration due to gravity on the surface of the planet in m/s2\text{m/s}^2?

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Cevap: 20

Cevap

The acceleration due to gravity on the surface of the planet is 20 m/s220\text{ m/s}^2.
The acceleration due to gravity at the surface of a spherical body is given by g=GMR2g = \frac{GM}{R^2}. When the mass is multiplied by 88 and the radius is multiplied by 22, the new acceleration becomes gp=G(8M)(2R)2=84GMR2=2gg_p = \frac{G(8M)}{(2R)^2} = \frac{8}{4}\frac{GM}{R^2} = 2g. Substituting g=10 m/s2g = 10\text{ m/s}^2 gives 20 m/s220\text{ m/s}^2.

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1
Write the expression for acceleration due to gravity at the surface of Earth.
ge=GMeRe2=10 m/s2g_e = \frac{GM_e}{R_e^2} = 10\text{ m/s}^2
Gravitational field strength at the surface depends directly on body mass and inversely on the square of radius.
2
Set up the ratio equation for the planet's gravitational acceleration using relative mass and radius values.
gp=G(8Me)(2Re)2=84(GMeRe2)=2geg_p = \frac{G(8M_e)}{(2R_e)^2} = \frac{8}{4} \left(\frac{GM_e}{R_e^2}\right) = 2g_e
Squaring the radius multiplier of 22 yields 44 in the denominator, while the numerator increases by a factor of 88.
3
Calculate the final numeric value.
gp=2×10 m/s2=20 m/s2g_p = 2 \times 10\text{ m/s}^2 = 20\text{ m/s}^2
Multiplying Earth's value by the combined ratio of 22 gives the answer.

Anahtar Kavram

Gravitational field strength on planetary surfaces (g=GMR2g = \frac{GM}{R^2})
Soru 1479Soru

A radioactive parent nucleus of Uranium-238 (92238U^{238}_{92}\text{U}) decays through a sequence of natural radioactive emissions to become a stable daughter nucleus of Lead-206 (82206Pb^{206}_{82}\text{Pb}). How many β\beta^--particles are emitted in total during this decay process?

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Cevap: 6

Cevap

6
The decrease in mass number from 238238 to 206206 is 3232, which corresponds to 88 alpha emissions (32/4=832 / 4 = 8). Emitting 88 alpha particles reduces the atomic number from 9292 to 7676 (9216=7692 - 16 = 76). To reach the atomic number of Lead (8282), the atomic number must be increased by 66 (8276=682 - 76 = 6), which requires emitting 66 beta-minus particles.

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1
Calculate the total change in mass number and deduce the number of alpha particles emitted.
The total mass number decreases by 238206=32238 - 206 = 32. Each alpha particle (24He^{4}_{2}\text{He}) decreases the mass number by 44, while beta particles have a mass number of 00. Therefore, the number of alpha particles is 324=8\frac{32}{4} = 8.
Beta particles carry negligible mass compared to nucleons, making alpha emission the sole mechanism for mass number reduction.
2
Calculate the intermediate atomic number after all alpha decays.
Each alpha particle removes 22 units of atomic number. The total reduction in atomic number due to 88 alpha particles is 8×2=168 \times 2 = 16. The intermediate atomic number is 9216=7692 - 16 = 76.
Alpha particles consist of 2 protons and 2 neutrons.
3
Determine the number of beta-minus particles required to reach the final atomic number.
The final atomic number of Lead-206 is 8282. The atomic number must increase by 8276=682 - 76 = 6. Since each β\beta^--particle increases the atomic number by 11, exactly 66 beta-minus particles are emitted.
A beta-minus decay converts a neutron into a proton, increasing the atomic number by 1 without altering the mass number.

Anahtar Kavram

Balancing mass numbers and atomic numbers in radioactive decay series
Soru 1480Soru

Two plane mirrors are inclined to each other at an angle of 6060^\circ. A ray of light strikes the first mirror at an angle of incidence of 4040^\circ and subsequently undergoes reflection at the second mirror. What is the total angle of deviation, in degrees, produced in the ray after the two successive reflections?

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Cevap: 240

Cevap

The total deviation produced in the light ray after successive reflections from both inclined plane mirrors is 240240^\circ.
When a light ray undergoes successive reflections at two plane mirrors inclined at an angle θ\theta, the total deviation DD experienced by the ray is given by D=3602θD = 360^\circ - 2\theta. Substituting θ=60\theta = 60^\circ yields D=3602(60)=240D = 360^\circ - 2(60^\circ) = 240^\circ. Step-by-step ray tracing confirms d1=1802(40)=100d_1 = 180^\circ - 2(40^\circ) = 100^\circ and d2=1802(20)=140d_2 = 180^\circ - 2(20^\circ) = 140^\circ, giving a total deviation of 100+140=240100^\circ + 140^\circ = 240^\circ.

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1
Calculate the deviation at the first mirror
d1=100d_1 = 100^\circ
The angle of deviation for a single reflection at a plane mirror is d=1802id = 180^\circ - 2i. For i1=40i_1 = 40^\circ, d1=18080=100d_1 = 180^\circ - 80^\circ = 100^\circ.
2
Find the angle of incidence on the second mirror using geometry
i2=20i_2 = 20^\circ
The glancing angle on the first mirror is g1=9040=50g_1 = 90^\circ - 40^\circ = 50^\circ. In the triangle formed by the ray path and the two mirrors inclined at 6060^\circ, the glancing angle on the second mirror is g2=180(60+50)=70g_2 = 180^\circ - (60^\circ + 50^\circ) = 70^\circ. Thus, the angle of incidence on the second mirror is i2=9070=20i_2 = 90^\circ - 70^\circ = 20^\circ.
3
Calculate the deviation at the second mirror and total deviation
d2=140d_2 = 140^\circ, D=240D = 240^\circ
The deviation at the second mirror is d2=1802(20)=140d_2 = 180^\circ - 2(20^\circ) = 140^\circ. Since both reflections rotate the ray in the same sense, the total deviation is D=d1+d2=100+140=240D = d_1 + d_2 = 100^\circ + 140^\circ = 240^\circ.

Anahtar Kavram

Total deviation produced by reflection from two inclined plane mirrors is independent of the initial angle of incidence and is given by D=3602θD = 360^\circ - 2\theta, where θ\theta is the angle of inclination between the mirrors.
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