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Question 7881Question

What is the value of 1log2100+1log5100\frac{1}{\log_2 100} + \frac{1}{\log_5 100}?

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Answer: 12\frac{1}{2}

Answer

12\frac{1}{2}
Using the change of base identity 1logab=logba\frac{1}{\log_a b} = \log_b a, the expression simplifies to log1002+log1005\log_{100} 2 + \log_{100} 5. By the product rule of logarithms, this equals log100(2×5)=log10010\log_{100}(2 \times 5) = \log_{100} 10. Since 10012=10100^{\frac{1}{2}} = 10, the value is 12\frac{1}{2}.

Step-by-Step Solution

1
Apply the reciprocal change of base rule 1logab=logba\frac{1}{\log_a b} = \log_b a.
1log2100=log1002\frac{1}{\log_2 100} = \log_{100} 2 and 1log5100=log1005\frac{1}{\log_5 100} = \log_{100} 5.
Converting to a common base of 100100 allows the use of logarithmic addition laws.
2
Combine the two logarithms using the product law logcx+logcy=logc(xy)\log_c x + \log_c y = \log_c (xy).
\log_{100} 2 + \log_{100} 5 = \log_{100} (2 \times 5) = \log_{100} 10.
Adding logarithms with the same base is equivalent to taking the logarithm of the product of their arguments.
3
Evaluate log10010\log_{100} 10.
Since 10012=10100^{\frac{1}{2}} = 10, log10010=12\log_{100} 10 = \frac{1}{2}.
The logarithm asks what power base 100100 must be raised to in order to equal 1010.

Key Concept

Logarithms and Change of Base
Estimated Time:1m 30s
Question 7882Question

A bag contains red, blue, and yellow marbles. The theoretical probability of selecting a red marble at random from the bag is 25\frac{2}{5}. In a probability experiment, a marble is drawn from the bag, its color recorded, and then replaced. This procedure is repeated 250250 times, resulting in a red marble being drawn 115115 times. What is the absolute difference between the observed experimental frequency of red marbles and the theoretical expected frequency?

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Answer: 15

Answer

15
The theoretical expected frequency of selecting a red marble over 250250 trials is found by multiplying the total trials by the theoretical probability: 250×25=100250 \times \frac{2}{5} = 100. The experimental frequency observed was 115115. Taking the absolute difference gives 115100=15|115 - 100| = 15.

Step-by-Step Solution

1
Calculate the theoretical expected frequency of red marble outcomes.
Theoretical expected frequency = 250×25=100250 \times \frac{2}{5} = 100.
Expected frequency is determined by multiplying the number of trials (N=250N = 250) by the theoretical probability (P=25P = \frac{2}{5}).
2
Find the absolute difference between the observed experimental frequency and the theoretical expected frequency.
115100=15|115 - 100| = 15.
The observed experimental frequency is 115115 and the theoretical expected frequency is 100100, so the positive difference is 1515.

Key Concept

Experimental Frequency vs. Theoretical Expected Frequency
Estimated Time:1m 30s
Question 7883Question

An unpolarized light beam with an initial intensity of 80 W/m280\text{ W/m}^2 passes through an ideal linear polarizer. What is the intensity of the transmitted light in W/m2\text{W/m}^2?

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Answer: 40

Answer

The intensity of the transmitted light is 40 W/m240\text{ W/m}^2.
When unpolarized light of initial intensity I0I_0 encounters an ideal linear polarizing filter, the transmitted intensity II is always equal to half of the incident intensity (I=12I0I = \frac{1}{2}I_0). Substituting 80 W/m280\text{ W/m}^2 gives I=40 W/m2I = 40\text{ W/m}^2.

Step-by-Step Solution

1
Determine the fraction of unpolarized light intensity transmitted by a polarizer.
Transmitted intensity formula I=12I0I = \frac{1}{2} I_0.
Unpolarized light consists of randomly oriented electric field vectors, resulting in an average transmission factor of one-half.
2
Substitute the incident intensity value into the formula.
I=802=40 W/m2I = \frac{80}{2} = 40\text{ W/m}^2.
Direct mathematical calculation.

Key Concept

Polarization and intensity reduction of unpolarized light upon passing through a linear polarizer.
Question 7884Question

A conductor wire with a cross-sectional area of 2.0×106m22.0 \times 10^{-6}\,\text{m}^2 carries a steady current of 1.6A1.6\,\text{A}. If the conduction electron density of the material is 5.0×1028m35.0 \times 10^{28}\,\text{m}^{-3} and the elementary charge is 1.6×1019C1.6 \times 10^{-19}\,\text{C}, what is the average drift velocity of the electrons in the wire?

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Answer: 1.0×104m/s1.0 \times 10^{-4}\,\text{m/s}

Answer

The average drift velocity of the electrons is 1.0×104m/s1.0 \times 10^{-4}\,\text{m/s}.
The correct answer is derived from the fundamental relationship I=nAevdI = n A e v_d. Solving for drift velocity gives vd=InAe=1.65.0×1028×2.0×106×1.6×1019=1.0×104m/sv_d = \frac{I}{n A e} = \frac{1.6}{5.0 \times 10^{28} \times 2.0 \times 10^{-6} \times 1.6 \times 10^{-19}} = 1.0 \times 10^{-4}\,\text{m/s}.

Step-by-Step Solution

1
Identify the drift velocity formula relating current to charge carrier parameters
The electric current is given by I=nAevdI = n A e v_d, where II is current, nn is electron density, AA is cross-sectional area, ee is elementary charge, and vdv_d is drift velocity.
This formula connects macroscopic electric current to microscopic charge dynamics.
2
Rearrange the equation to solve for drift velocity vdv_d
vd=InAev_d = \frac{I}{n A e}
Isolating the unknown variable vdv_d before substituting known values.
3
Substitute the given values into the expression
vd=1.6(5.0×1028)×(2.0×106)×(1.6×1019)v_d = \frac{1.6}{(5.0 \times 10^{28}) \times (2.0 \times 10^{-6}) \times (1.6 \times 10^{-19})}
Inserting I=1.6AI = 1.6\,\text{A}, n=5.0×1028m3n = 5.0 \times 10^{28}\,\text{m}^{-3}, A=2.0×106m2A = 2.0 \times 10^{-6}\,\text{m}^2, and e=1.6×1019Ce = 1.6 \times 10^{-19}\,\text{C}.
4
Evaluate the denominator and compute the final value of vdv_d
Denominator =(5.0×2.0×1.6)×1028619=16.0×103=1.6×104= (5.0 \times 2.0 \times 1.6) \times 10^{28 - 6 - 19} = 16.0 \times 10^3 = 1.6 \times 10^4. Thus, vd=1.61.6×104=1.0×104m/sv_d = \frac{1.6}{1.6 \times 10^4} = 1.0 \times 10^{-4}\,\text{m/s}.
Simplifying powers of ten gives the final numerical answer.

Key Concept

Relationship between Electric Current and Drift Velocity
Estimated Time:1m 30s
Question 7885Question

A liquid has a density of 840 kg m3840\text{ kg m}^{-3} at 10C10^\circ\text{C}. It is heated inside a container whose material has a linear expansivity of 2.0×105 K12.0 \times 10^{-5}\text{ K}^{-1}. If the measured apparent cubic expansivity of the liquid in this container is 4.4×104 K14.4 \times 10^{-4}\text{ K}^{-1}, what is the density of the liquid at 110C110^\circ\text{C} in kg m3\text{kg m}^{-3}?

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Answer: 800

Answer

800 kg m^-3
To find the density of the liquid at the elevated temperature, we must use its real cubic expansivity γr\gamma_r. The vessel expands with a cubic expansivity of γv=3α=6.0×105 K1\gamma_v = 3\alpha = 6.0 \times 10^{-5}\text{ K}^{-1}. The real cubic expansivity of the liquid is γr=γa+γv=4.4×104+0.6×104=5.0×104 K1\gamma_r = \gamma_a + \gamma_v = 4.4 \times 10^{-4} + 0.6 \times 10^{-4} = 5.0 \times 10^{-4}\text{ K}^{-1}. Using the density variation formula ρ2=ρ11+γrΔT\rho_2 = \frac{\rho_1}{1 + \gamma_r \Delta T}, we evaluate 8401+(5.0×104×100)=8401.05=800 kg m3\frac{840}{1 + (5.0 \times 10^{-4} \times 100)} = \frac{840}{1.05} = 800\text{ kg m}^{-3}.

Step-by-Step Solution

1
Calculate the cubic expansivity of the container material
γv=6.0×105 K1\gamma_v = 6.0 \times 10^{-5}\text{ K}^{-1}
The volume (cubic) expansivity of a solid container is three times its linear expansivity (γv=3α\gamma_v = 3\alpha).
2
Determine the real cubic expansivity of the liquid
γr=5.0×104 K1\gamma_r = 5.0 \times 10^{-4}\text{ K}^{-1}
The real cubic expansivity is the sum of the apparent cubic expansivity and the cubic expansivity of the container (γr=γa+γv\gamma_r = \gamma_a + \gamma_v).
3
Determine the change in temperature
ΔT=100 K\Delta T = 100\text{ K}
Subtract the initial temperature from the final temperature: 110C10C=100 K110^\circ\text{C} - 10^\circ\text{C} = 100\text{ K}.
4
Calculate the final density of the liquid at 110C110^\circ\text{C}
ρ2=800 kg m3\rho_2 = 800\text{ kg m}^{-3}
Density varies inversely with volumetric expansion according to ρ2=ρ11+γrΔT\rho_2 = \frac{\rho_1}{1 + \gamma_r \Delta T}.

Key Concept

Relationship between real expansivity, apparent expansivity, container expansion, and density change in fluids
Question 7886Question

A research rocket is launched vertically upwards from rest with a constant acceleration of 5.0 m/s25.0\text{ m/s}^2. At an altitude of 250 m250\text{ m}, its engine suddenly fails and the rocket continues to move vertically upward under gravity alone. Calculate the total time, in seconds, taken by the rocket from launch until it reaches its maximum height. (Take acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2)

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Answer: 15

Answer

The total time taken from launch to reach maximum height is 15 s15\text{ s}.
The motion occurs in two phases. In phase 1, accelerating uniformly from rest at 5.0 m/s25.0\text{ m/s}^2 over 250 m250\text{ m} yields a velocity of 50 m/s50\text{ m/s} in 10 s10\text{ s}. In phase 2, moving upward under gravity alone (10 m/s210\text{ m/s}^2) reduces the velocity from 50 m/s50\text{ m/s} to rest (0 m/s0\text{ m/s}) in 5 s5\text{ s}. Adding the durations of both phases gives 10 s+5 s=15 s10\text{ s} + 5\text{ s} = 15\text{ s}.

Step-by-Step Solution

1
Calculate the rocket's velocity and elapsed time at the moment of engine failure.
Velocity v1=50 m/sv_1 = 50\text{ m/s} and time t1=10 st_1 = 10\text{ s}.
The rocket accelerates uniformly from rest at 5.0 m/s25.0\text{ m/s}^2 over a distance of 250 m250\text{ m}.
2
Calculate the duration of the unpowered upward motion until vertical velocity becomes zero.
Unpowered flight time t2=5 st_2 = 5\text{ s}.
After engine failure, the rocket acts as a free projectile moving upward against gravity (g=10 m/s2g = 10\text{ m/s}^2) with an initial velocity of 50 m/s50\text{ m/s}.
3
Sum the time intervals of both stages.
Total time ttotal=10 s+5 s=15 st_{\text{total}} = 10\text{ s} + 5\text{ s} = 15\text{ s}.
The total motion consists of two distinct stages: powered acceleration followed by gravitational deceleration.

Key Concept

Multi-stage vertical motion under constant acceleration followed by free-fall under gravity
Question 7887Question

The energy density uu (defined as energy per unit volume) stored in an electrostatic field is related to the permittivity of free space ϵ0\epsilon_0 and the electric field strength EE by the dimensional formula u=kϵ0xEyu = k \epsilon_0^x E^y, where kk is a dimensionless constant. What is the value of the numerical exponent yy?

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Answer: 2

Answer

The value of the exponent yy is 2.
By writing the dimensions of energy density [ML1T2][M L^{-1} T^{-2}], permittivity [M1L3T4I2][M^{-1} L^{-3} T^4 I^2], and electric field strength [MLT3I1][M L T^{-3} I^{-1}], equating powers of electric current II yields 2xy=02x - y = 0 (or y=2xy = 2x). Substituting this into the equation for powers of mass MM, x+y=1-x + y = 1, yields x+2x=1-x + 2x = 1, so x=1x = 1 and y=2y = 2.

Step-by-Step Solution

1
Derive the dimensional formulas for energy density uu, permittivity ϵ0\epsilon_0, and electric field EE.
[u] = M L^{-1} T^{-2}, [\epsilon_0] = M^{-1} L^{-3} T^4 I^2, [E] = M L T^{-3} I^{-1}.
Expressing quantities in terms of base dimensions (M, L, T, I) is required for dimensional homogeneity.
2
Form the dimensional equation u=kϵ0xEyu = k \epsilon_0^x E^y and combine powers.
M L^{-1} T^{-2} = M^{-x+y} L^{-3x+y} T^{4x-3y} I^{2x-y}.
Applies the principle of dimensional consistency across the formula.
3
Equate corresponding powers of base dimensions to set up equations for xx and yy.
For I: 2x - y = 0; for M: -x + y = 1.
Base unit exponents on both sides of a physically valid equation must match.
4
Solve the algebraic equations for the unknown exponent yy.
x = 1, y = 2.
Substituting y = 2x into -x + y = 1 directly gives x = 1 and y = 2.

Key Concept

Dimensional Analysis and Dimensional Homogeneity
Estimated Time:1m 30s
Question 7888Question

A rifle of mass 4.0 kg4.0\text{ kg} fires a bullet of mass 0.01 kg0.01\text{ kg} with a velocity of 400 m s1400\text{ m s}^{-1}. What is the recoil velocity of the rifle?

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Answer: 1.0 m s1-1.0\text{ m s}^{-1}

Answer

The recoil velocity of the rifle is 1.0 m s1-1.0\text{ m s}^{-1} (or 1.0 m s11.0\text{ m s}^{-1} in the direction opposite to the bullet).
The system starts at rest, so the initial total momentum is zero. By the law of conservation of linear momentum, the total final momentum must also be zero: mriflevrifle+mbulletvbullet=0m_{rifle}v_{rifle} + m_{bullet}v_{bullet} = 0. Substituting mrifle=4.0 kgm_{rifle} = 4.0\text{ kg}, mbullet=0.01 kgm_{bullet} = 0.01\text{ kg}, and vbullet=400 m s1v_{bullet} = 400\text{ m s}^{-1} gives 4.0vrifle+4.0=04.0 v_{rifle} + 4.0 = 0, which yields vrifle=1.0 m s1v_{rifle} = -1.0\text{ m s}^{-1}. The negative sign indicates that the rifle moves in the direction opposite to the bullet.

Step-by-Step Solution

1
State the principle of conservation of linear momentum
Total Initial Momentum = Total Final Momentum = 0
Before firing, both the rifle and bullet are at rest.
2
Set up the linear momentum conservation equation
mriflevrifle+mbulletvbullet=0m_{rifle} v_{rifle} + m_{bullet} v_{bullet} = 0
The sum of the final momenta of the system components must equal zero.
3
Substitute the given numerical values into the equation and solve for recoil velocity
4.0vrifle+(0.01400)=0    4.0vrifle+4=0    vrifle=1.0 m s14.0 \cdot v_{rifle} + (0.01 \cdot 400) = 0 \implies 4.0 \cdot v_{rifle} + 4 = 0 \implies v_{rifle} = -1.0\text{ m s}^{-1}
Solving the linear algebraic equation yields the exact magnitude and direction of the recoil velocity.

Key Concept

Law of Conservation of Linear Momentum and Newton's Third Law of Motion
Estimated Time:45s
Question 7889Question

What is the positive value of xx that satisfies the equation 22x+192x+4=02^{2x+1} - 9 \cdot 2^x + 4 = 0?

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Answer: 2

Answer

The positive value of xx that satisfies the equation is 2.
Applying the law of indices am+n=amana^{m+n} = a^m \cdot a^n gives 22x+1=2(2x)22^{2x+1} = 2 \cdot (2^x)^2. Setting y=2xy = 2^x yields the quadratic equation 2y29y+4=02y^2 - 9y + 4 = 0. Factoring this expression gives (2y1)(y4)=0(2y - 1)(y - 4) = 0, which yields roots y=12y = \frac{1}{2} and y=4y = 4. Solving 2x=122^x = \frac{1}{2} gives x=1x = -1, and solving 2x=42^x = 4 gives x=2x = 2. The positive value is 22.

Step-by-Step Solution

1
Use index laws to express the equation in terms of 2x2^x
2(2x)29(2x)+4=02 \cdot (2^x)^2 - 9 \cdot (2^x) + 4 = 0
By the product law of indices, 22x+1=22x21=2(2x)22^{2x+1} = 2^{2x} \cdot 2^1 = 2 \cdot (2^x)^2.
2
Substitute y=2xy = 2^x to form a quadratic equation
2y29y+4=02y^2 - 9y + 4 = 0
Replacing 2x2^x with a single variable simplifies the exponential equation into quadratic form.
3
Solve the quadratic equation for yy
y=12y = \frac{1}{2} or y=4y = 4
Factoring 2y29y+4=02y^2 - 9y + 4 = 0 gives (2y1)(y4)=0(2y - 1)(y - 4) = 0.
4
Substitute back y=2xy = 2^x to solve for xx
x=1x = -1 or x=2x = 2
Since 2x=12=212^x = \frac{1}{2} = 2^{-1}, x=1x = -1. Since 2x=4=222^x = 4 = 2^2, x=2x = 2.
5
Select the positive value requested by the question
x=2x = 2
x=2x = 2 is positive, whereas x=1x = -1 is negative.

Key Concept

Reducing exponential equations to quadratic form using index laws
Estimated Time:1m 30s
Question 7890Question

Determine the smallest integer value of xx that satisfies the compound inequality 3<2x5113 < 2x - 5 \le 11.

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Answer: 5

Answer

The smallest integer value of xx that satisfies the inequality is 5.
Adding 5 across the compound inequality 3<2x5113 < 2x - 5 \le 11 gives 8<2x168 < 2x \le 16. Dividing by 2 yields 4<x84 < x \le 8. The integer values satisfying this range are 5, 6, 7, and 8. Therefore, the smallest integer solution is 5.

Step-by-Step Solution

1
Add 5 to all parts of the compound inequality
8 < 2x <= 16
Isolates the variable term in the middle segment.
2
Divide all parts of the compound inequality by 2
4 < x <= 8
Solves for x without changing inequality signs since 2 is positive.
3
Identify integer solutions within the range (4, 8]
x in {5, 6, 7, 8}
Since the inequality at 4 is strict (<), 4 is excluded, but 8 is included (<=).
4
Find the minimum integer value in the solution set
5
5 is the smallest integer strictly greater than 4.

Key Concept

Solving Compound Linear Inequalities
Question 7891Question

A steel rod and a brass rod are arranged such that the difference between their lengths remains constant at 10 cm10\text{ cm} at all temperatures. If the linear expansivity of steel is 1.2×105 K11.2 \times 10^{-5}\text{ K}^{-1} and that of brass is 1.8×105 K11.8 \times 10^{-5}\text{ K}^{-1}, what is the initial length of the steel rod in centimetres?

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Answer: 30

Answer

The initial length of the steel rod is 30 cm30\text{ cm}.
For the length difference between two rods to remain constant regardless of temperature change, both rods must undergo equal absolute expansion (\(\Delta L_1 = \Delta L_2\)). Since \(\Delta L = L_0 \alpha \Delta T\), this requires \(L_1 \alpha_1 = L_2 \alpha_2\). Substituting \(L_{\text{brass}} = L_{\text{steel}} - 10\text{ cm}\) and the given expansivity values gives \(1.2 \times 10^{-5} L_{\text{steel}} = 1.8 \times 10^{-5} (L_{\text{steel}} - 10)\), which simplifies to \(0.6 L_{\text{steel}} = 18\), giving \(L_{\text{steel}} = 30\text{ cm}\).

Step-by-Step Solution

1
Relate the condition for a constant difference in length to individual expansions
\(\Delta L_{\text{steel}} = \Delta L_{\text{brass}}\)
If the difference between the two lengths is constant across temperature changes, both rods must increase in length by the exact same amount for any given temperature change.
2
Apply the linear thermal expansion formula to both rods
\(L_{\text{steel}} \alpha_{\text{steel}} = L_{\text{brass}} \alpha_{\text{brass}}\)
Since \(\Delta L = L_0 \alpha \Delta T\), setting \(\Delta L_{\text{steel}} = \Delta L_{\text{brass}}\) gives \(L_{\text{steel}} \alpha_{\text{steel}} \Delta T = L_{\text{brass}} \alpha_{\text{brass}} \Delta T\). Cancelling \(\Delta T\) yields \(L_{\text{steel}} \alpha_{\text{steel}} = L_{\text{brass}} \alpha_{\text{brass}}\).
3
Substitute the length relationship into the equation
\(L_{\text{steel}} (1.2 \times 10^{-5}) = (L_{\text{steel}} - 10) (1.8 \times 10^{-5})\)
Because brass has a larger linear expansivity than steel, the brass rod must be shorter than the steel rod so that their products of length and expansivity remain equal, hence \(L_{\text{brass}} = L_{\text{steel}} - 10\text{ cm}\).
4
Solve for the length of the steel rod
\(L_{\text{steel}} = 30\text{ cm}\)
Dividing both sides by \(10^{-5}\) gives \(1.2 L_{\text{steel}} = 1.8 L_{\text{steel}} - 18\). Rearranging gives \(0.6 L_{\text{steel}} = 18\), which yields \(L_{\text{steel}} = \frac{18}{0.6} = 30\text{ cm}\).

Key Concept

Equal absolute linear expansion for constant length difference
Estimated Time:2m 0s
Question 7892Question

A point P(x,y)P(x, y) moves in the Cartesian plane such that it maintains a constant distance of 10 units10\text{ units} from a fixed point C(2,3)C(2, -3). If the locus of PP intersects the vertical line x=8x = 8 at two points AA and BB, what is the distance between AA and BB?

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Answer: 16

Answer

The distance between the intersection points A and B is 16 units.
The locus of point P moving at a constant distance of 10 units from C(2, -3) forms a circle (x2)2+(y+3)2=100(x - 2)^2 + (y + 3)^2 = 100. Substituting x=8x = 8 yields (y+3)2=64(y + 3)^2 = 64, giving y=5y = 5 and y=11y = -11. The distance between the two points (8, 5) and (8, -11) along the vertical line x=8x = 8 is 5(11)=165 - (-11) = 16 units.

Step-by-Step Solution

1
Determine the equation representing the locus of point P
(x2)2+(y+3)2=100(x - 2)^2 + (y + 3)^2 = 100
The locus of a point moving at a fixed distance from a fixed point is a circle with equation (xh)2+(yk)2=r2(x - h)^2 + (y - k)^2 = r^2.
2
Substitute x=8x = 8 into the locus equation to find the yy-coordinates of the intersection points
(82)2+(y+3)2=100    36+(y+3)2=100    (y+3)2=64(8 - 2)^2 + (y + 3)^2 = 100 \implies 36 + (y + 3)^2 = 100 \implies (y + 3)^2 = 64
The intersection points lie on both the locus circle and the vertical line x=8x = 8.
3
Solve for the two possible values of yy
y+3=±8    y1=5y + 3 = \pm 8 \implies y_1 = 5 and y2=11y_2 = -11
Taking the square root gives both positive and negative solutions for the vertical coordinate.
4
Calculate the vertical distance between points A(8,5)A(8, 5) and B(8,11)B(8, -11)
Distance=5(11)=16 units\text{Distance} = 5 - (-11) = 16\text{ units}
Since both points have the same xx-coordinate (x=8x = 8), the distance is simply the absolute difference between their yy-coordinates.

Key Concept

Locus of a point at a constant distance from a fixed point (Circle)
Question 7893Question

Match each length measuring instrument listed on the left with its standard precision or suitable measurement application on the right.

Click a left item, then click its matching right item

Items

Micrometer screw gauge
Vernier caliper
Metre rule
Tape measure

Matches

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Answer

Micrometer screw gauge matches with precision 0.01 mm0.01\text{ mm} for fine wire diameter; Vernier caliper matches with precision 0.01 cm0.01\text{ cm} for tube diameters; Metre rule matches with precision 0.1 cm0.1\text{ cm} for laboratory lengths; Tape measure matches with flexible long-distance measuring.
Each instrument is correctly matched to its standard least count and characteristic physical measurement task: Micrometer screw gauge (0.01 mm0.01\text{ mm}), Vernier caliper (0.01 cm0.01\text{ cm}), Metre rule (0.1 cm0.1\text{ cm}), and Tape measure for long flexible lengths.

Step-by-Step Solution

1
Identify the least count and primary application for each measuring tool.
Micrometer screw gauge: 0.01 mm0.01\text{ mm} (wires); Vernier caliper: 0.01 cm0.01\text{ cm} (internal/external tube diameters); Metre rule: 0.1 cm0.1\text{ cm} (standard lab objects); Tape measure: large flexible distances.
Matching instruments requires recalling their resolution (least count) and physical design features.

Key Concept

Instrument least counts and appropriate selection based on object dimensions.
Question 7894Question

A shell is launched from level ground into the air. It reaches a maximum height of 45 m45\text{ m} above the ground and has a total horizontal range of 240 m240\text{ m}. Taking g=10 m/s2g = 10\text{ m/s}^2, calculate the magnitude of the initial launch velocity of the shell in m/s\text{m/s}.

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Answer: 50

Answer

The initial launch velocity of the shell is 50 m/s50\text{ m/s}.
Combining the expressions for maximum height H=u2sin2θ2gH = \frac{u^2\sin^2\theta}{2g} and range R=2u2sinθcosθgR = \frac{2u^2\sin\theta\cos\theta}{g} gives tanθ=4HR\tan\theta = \frac{4H}{R}. With H=45 mH = 45\text{ m} and R=240 mR = 240\text{ m}, we get tanθ=0.75=34\tan\theta = 0.75 = \frac{3}{4}, which yields sinθ=0.6\sin\theta = 0.6. Substituting these into the height equation yields 45=u2(0.6)22045 = \frac{u^2(0.6)^2}{20}, solving to u=50 m/su = 50\text{ m/s}.

Step-by-Step Solution

1
Express the launch angle in terms of maximum height and horizontal range
\tan\theta = \frac{4H}{R} = \frac{4 \times 45}{240} = 0.75
Dividing the maximum height formula H=u2sin2θ2gH = \frac{u^2\sin^2\theta}{2g} by the horizontal range formula R=2u2sinθcosθgR = \frac{2u^2\sin\theta\cos\theta}{g} yields HR=14tanθ\frac{H}{R} = \frac{1}{4}\tan\theta.
2
Find the sine of the launch angle from the tangent value
sinθ=0.6\sin\theta = 0.6
For a right-angled triangle with tanθ=34\tan\theta = \frac{3}{4}, the hypotenuse is 32+42=5\sqrt{3^2 + 4^2} = 5, giving sinθ=35=0.6\sin\theta = \frac{3}{5} = 0.6.
3
Calculate the magnitude of the initial velocity uu
u = 50\text{ m/s}
Substituting values into H=u2sin2θ2gH = \frac{u^2\sin^2\theta}{2g} gives 45=u2(0.6)22(10)    900=0.36u2    u=50 m/s45 = \frac{u^2 (0.6)^2}{2(10)} \implies 900 = 0.36 u^2 \implies u = 50\text{ m/s}.

Key Concept

Interdependence of Maximum Height, Range, and Launch Velocity in Projectile Motion
Estimated Time:1m 30s
Question 7895Question

The table below shows the distribution of test scores obtained by a group of students:

Score12345
Frequency3xx421

If the mean score of the distribution is 2.52.5, what is the median score?

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Answer: 22

Answer

The median score is 22.
First, calculate the missing frequency xx using the mean formula xˉ=fxf=28+2x10+x=2.5\bar{x} = \frac{\sum fx}{\sum f} = \frac{28 + 2x}{10 + x} = 2.5, which yields x=6x = 6. Total number of scores is N=16N = 16. The median is the mean of the 8th8\text{th} and 9th9\text{th} values. Looking at cumulative frequencies, score 1 covers positions 1–3 and score 2 covers positions 4–9. Thus, both the 8th8\text{th} and 9th9\text{th} scores are 2, giving a median of 2.

Step-by-Step Solution

1
Set up the equation for the mean using xˉ=fxf\bar{x} = \frac{\sum fx}{\sum f}.
Total frequency f=3+x+4+2+1=10+x\sum f = 3 + x + 4 + 2 + 1 = 10 + x, and total score sum fx=1(3)+2(x)+3(4)+4(2)+5(1)=28+2x\sum fx = 1(3) + 2(x) + 3(4) + 4(2) + 5(1) = 28 + 2x.
The mean of an ungrouped frequency distribution is the sum of all score-frequency products divided by the total frequency.
2
Solve for the unknown frequency xx.
2.5=28+2x10+x    2.5(10+x)=28+2x    25+2.5x=28+2x    0.5x=3    x=62.5 = \frac{28 + 2x}{10 + x} \implies 2.5(10 + x) = 28 + 2x \implies 25 + 2.5x = 28 + 2x \implies 0.5x = 3 \implies x = 6.
Equating the mean expression to 2.52.5 gives the value of xx.
3
Find total number of observations NN and determine the median position.
N=10+6=16N = 10 + 6 = 16. Since NN is even, median position is between the 8th8\text{th} and 9th9\text{th} values.
For an even number of observations NN, the median is the average of the N2th\frac{N}{2}\text{th} and (N2+1)th(\frac{N}{2} + 1)\text{th} items.
4
Locate the 8th8\text{th} and 9th9\text{th} items using cumulative frequencies.
Cumulative frequencies: Score 1 has 3; Score 2 reaches 3+6=93 + 6 = 9. Both the 8th8\text{th} and 9th9\text{th} values are 22. Therefore, median =2+22=2= \frac{2 + 2}{2} = 2.
Positions 4 through 9 correspond to the score 22.

Key Concept

Measures of central tendency for ungrouped frequency distributions
Question 7896Question

A body starting from rest accelerates uniformly along a straight path at a rate of 2.5 m/s22.5\text{ m/s}^2. What is the distance covered by the body in 4.0 s4.0\text{ s}?

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Answer: 20 m20\text{ m}

Answer

The distance covered by the body in 4.0 s4.0\text{ s} is 20 m20\text{ m}.
Using the kinematic relation s=ut+12at2s = ut + \frac{1}{2}at^2 with u=0 m/su = 0\text{ m/s}, a=2.5 m/s2a = 2.5\text{ m/s}^2, and t=4.0 st = 4.0\text{ s} gives s=0+12×2.5×(4.0)2=20 ms = 0 + \frac{1}{2} \times 2.5 \times (4.0)^2 = 20\text{ m}.

Step-by-Step Solution

1
Identify the given kinematic values.
Initial velocity u=0 m/su = 0\text{ m/s}, acceleration a=2.5 m/s2a = 2.5\text{ m/s}^2, and time t=4.0 st = 4.0\text{ s}.
The problem states the body starts from rest and undergoes uniform linear acceleration.
2
Select the appropriate formula for distance under uniform acceleration.
s=ut+12at2s = ut + \frac{1}{2}at^2
This equation connects initial velocity, acceleration, elapsed time, and total displacement.
3
Substitute the given values into the equation and compute displacement.
s=(0)(4.0)+12(2.5)(4.0)2=0.5×2.5×16=20 ms = (0)(4.0) + \frac{1}{2}(2.5)(4.0)^2 = 0.5 \times 2.5 \times 16 = 20\text{ m}.
Evaluating the expressions yields the distance traveled in meters.

Key Concept

Kinematic Equation for Linear Distance Under Uniform Acceleration
Estimated Time:45s
Question 7897Question

A beam of cathode rays (electrons) traveling at a speed of 4.00×106 m s14.00 \times 10^{6}\text{ m s}^{-1} enters a region with a uniform magnetic field of 5.00×104 T5.00 \times 10^{-4}\text{ T} directed perpendicular to the beam. Taking the specific charge of an electron (em\frac{e}{m}) to be 1.60×1011 C kg11.60 \times 10^{11}\text{ C kg}^{-1}, what is the radius of the circular path traced by the cathode rays, in centimeters?

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Answer: 5

Answer

The radius of the circular path followed by the cathode rays is 5.0 cm.
When cathode rays enter a uniform magnetic field at right angles, the magnetic force acts as a centripetal force causing the electron beam to trace a circular arc of radius r=v(e/m)Br = \frac{v}{(e/m)B}. Substituting v=4.00×106 m s1v = 4.00 \times 10^6\text{ m s}^{-1}, e/m=1.60×1011 C kg1e/m = 1.60 \times 10^{11}\text{ C kg}^{-1}, and B=5.00×104 TB = 5.00 \times 10^{-4}\text{ T} yields r=0.05 mr = 0.05\text{ m}, which equals 5.0 cm5.0\text{ cm}.

Step-by-Step Solution

1
Set the magnetic Lorentz force equal to the required centripetal force for circular motion.
evB=mv2re v B = \frac{m v^2}{r}
Cathode rays consist of moving electrons experiences a magnetic force perpendicular to both their velocity and the magnetic field.
2
Express the radius rr in terms of speed vv, magnetic field BB, and specific charge em\frac{e}{m}.
r=v(em)Br = \frac{v}{\left(\frac{e}{m}\right) B}
Simplifying the force balance equation isolates the radius on one side.
3
Substitute the given numerical values into the expression for rr.
r=4.00×106 m s1(1.60×1011 C kg1)×(5.00×104 T)=0.05 mr = \frac{4.00 \times 10^{6}\text{ m s}^{-1}}{\left(1.60 \times 10^{11}\text{ C kg}^{-1}\right) \times \left(5.00 \times 10^{-4}\text{ T}\right)} = 0.05\text{ m}
Calculating the denominator gives 8.00×107 C T kg18.00 \times 10^{7}\text{ C T kg}^{-1}, leading to 0.05 m0.05\text{ m}.
4
Convert the radius from meters to centimeters as requested by the question.
r=0.05 m×100 cm m1=5.0 cmr = 0.05\text{ m} \times 100\text{ cm m}^{-1} = 5.0\text{ cm}
1 meter equals 100 centimeters.

Key Concept

Deflection of Cathode Rays in a Magnetic Field
Estimated Time:1m 30s
Question 7898Question

A pneumatic cylinder in a hydraulic brake mechanism contains 0.050 m30.050\text{ m}^3 of an ideal gas at an initial pressure of 1.20×105 Pa1.20 \times 10^5\text{ Pa} and a temperature of 27C27^\circ\text{C}. The gas is first compressed isothermally to a volume of 0.020 m30.020\text{ m}^3, and then heated at constant volume until its pressure reaches 6.00×105 Pa6.00 \times 10^5\text{ Pa}. What is the final temperature of the gas in degrees Celsius?

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Answer: 327C327^\circ\text{C}

Answer

The final temperature of the gas is 327C327^\circ\text{C}.
First, converting the initial temperature gives T1=27C+273=300 KT_1 = 27^\circ\text{C} + 273 = 300\text{ K}. For the isothermal compression, the pressure increases to P2=P1×V1V2=1.20×105×0.0500.020=3.00×105 PaP_2 = P_1 \times \frac{V_1}{V_2} = 1.20 \times 10^5 \times \frac{0.050}{0.020} = 3.00 \times 10^5\text{ Pa}. Next, during the constant volume heating step to P3=6.00×105 PaP_3 = 6.00 \times 10^5\text{ Pa}, the pressure doubles, requiring the absolute temperature to double from 300 K300\text{ K} to 600 K600\text{ K}. Converting 600 K600\text{ K} back to Celsius yields 600273=327C600 - 273 = 327^\circ\text{C}.

Step-by-Step Solution

1
Convert the initial temperature from Celsius to Kelvin.
T1=27+273=300 KT_1 = 27 + 273 = 300\text{ K}.
Gas laws strictly require thermodynamic temperatures expressed in Kelvin.
2
Apply Boyle's Law (P1V1=P2V2P_1 V_1 = P_2 V_2) to determine the intermediate pressure P2P_2 after isothermal compression at constant temperature T2=300 KT_2 = 300\text{ K}.
P2=P1V1V2=(1.20×105 Pa)(0.050 m3)0.020 m3=3.00×105 PaP_2 = \frac{P_1 V_1}{V_2} = \frac{(1.20 \times 10^5\text{ Pa})(0.050\text{ m}^3)}{0.020\text{ m}^3} = 3.00 \times 10^5\text{ Pa}.
During an isothermal process, the product of pressure and volume remains constant.
3
Apply Pressure Law (Gay-Lussac's Law) for the second stage, where volume remains constant (V3=V2=0.020 m3V_3 = V_2 = 0.020\text{ m}^3) while pressure increases from P2=3.00×105 PaP_2 = 3.00 \times 10^5\text{ Pa} to P3=6.00×105 PaP_3 = 6.00 \times 10^5\text{ Pa}.
P2T2=P3T3    T3=T2×P3P2=300 K×6.00×105 Pa3.00×105 Pa=600 K\frac{P_2}{T_2} = \frac{P_3}{T_3} \implies T_3 = T_2 \times \frac{P_3}{P_2} = 300\text{ K} \times \frac{6.00 \times 10^5\text{ Pa}}{3.00 \times 10^5\text{ Pa}} = 600\text{ K}.
At constant volume, pressure is directly proportional to absolute temperature.
4
Convert the final temperature T3T_3 back to degrees Celsius.
t3=600273=327Ct_3 = 600 - 273 = 327^\circ\text{C}.
The question explicitly requests the final temperature in degrees Celsius.

Key Concept

Multi-stage gas processes combining Boyle's Law and Pressure Law using the Ideal Gas Equation
Question 7899Question

How many distinct solutions exist for the trigonometric equation 2cos2θ=12\cos 2\theta = 1 within the interval 0θ3600^\circ \le \theta \le 360^\circ?

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Answer: 4

Answer

4 distinct solutions
The equation cos2θ=12\cos 2\theta = \frac{1}{2} requires finding all angles whose cosine is 12\frac{1}{2}. Because the angle argument is 2θ2\theta, as θ\theta completes one full rotation (00^\circ to 360360^\circ), 2θ2\theta completes two full rotations (00^\circ to 720720^\circ). In two rotations, the cosine function takes the value +12+\frac{1}{2} exactly four times (twice per rotation), leading to four distinct solutions for θ\theta.

Step-by-Step Solution

1
Isolate the trigonometric function in the equation
cos2θ=12\cos 2\theta = \frac{1}{2}
Dividing both sides by 2 isolates the cosine term.
2
Determine the working interval for the multiple angle 2θ2\theta
02θ7200^\circ \le 2\theta \le 720^\circ
Since 0θ3600^\circ \le \theta \le 360^\circ, multiplying the inequality by 2 gives the domain for 2θ2\theta.
3
Find all values of 2θ2\theta where cosine is positive 12\frac{1}{2} in the domain [0,720][0^\circ, 720^\circ]
2θ=60,300,420,6602\theta = 60^\circ, 300^\circ, 420^\circ, 660^\circ
Cosine is positive in Quadrants I and IV. In the first revolution (0 to 3600^\circ \text{ to } 360^\circ), 2θ=602\theta = 60^\circ and 36060=300360^\circ - 60^\circ = 300^\circ. Adding 360360^\circ for the second revolution gives 420420^\circ and 660660^\circ.
4
Solve for θ\theta by dividing each angle by 2
θ=30,150,210,330\theta = 30^\circ, 150^\circ, 210^\circ, 330^\circ
Dividing all four values of 2θ2\theta by 2 gives four distinct values of θ\theta within [0,360][0^\circ, 360^\circ].

Key Concept

Solving trigonometric equations with multiple angles over a specified domain
Question 7900Question

In electrostatics, Coulomb's law states that the force FF between two point charges q1q_1 and q2q_2 separated by a distance rr in a vacuum is given by F=q1q24πε0r2F = \frac{q_1 q_2}{4\pi \varepsilon_0 r^2}, where ε0\varepsilon_0 is the permittivity of free space. What are the fundamental dimensions of ε0\varepsilon_0 expressed in terms of mass (MM), length (LL), time (TT), and electric current (II)?

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Answer: M1L3T4I2M^{-1} L^{-3} T^4 I^2

Answer

The dimensions of permittivity of free space ε0\varepsilon_0 are M1L3T4I2M^{-1} L^{-3} T^4 I^2.
The correct answer is derived by isolating ε0=q1q24πFr2\varepsilon_0 = \frac{q_1 q_2}{4\pi F r^2}. Substituting [q]=IT[q] = I T, [F]=MLT2[F] = M L T^{-2}, and [r]=L[r] = L gives [ε0]=I2T2ML3T2=M1L3T4I2[\varepsilon_0] = \frac{I^2 T^2}{M L^3 T^{-2}} = M^{-1} L^{-3} T^4 I^2.

Step-by-Step Solution

1
Rearrange Coulomb's Law to isolate permittivity of free space ε0\varepsilon_0
ε0=q1q24πFr2\varepsilon_0 = \frac{q_1 q_2}{4\pi F r^2}
Isolating ε0\varepsilon_0 allows us to substitute the dimensions of each constituent physical quantity.
2
Determine the dimensions of charge qq, force FF, distance rr, and the constant 4π4\pi
[q]=IT[q] = I T, [F]=MLT2[F] = M L T^{-2}, [r2]=L2[r^2] = L^2, and [4π]=1[4\pi] = 1 (dimensionless)
Electric current is a base unit (II), so electric charge is current multiplied by time (ITI T). Force is mass times acceleration (MLT2M L T^{-2}).
3
Substitute the fundamental dimensions into the rearranged equation and simplify exponent powers
[ε0]=(IT)(IT)(MLT2)(L2)=I2T2ML3T2=M1L3T4I2[\varepsilon_0] = \frac{(I T)(I T)}{(M L T^{-2})(L^2)} = \frac{I^2 T^2}{M L^3 T^{-2}} = M^{-1} L^{-3} T^4 I^2
Applying exponent laws: T2/T2=T2(2)=T4T^2 / T^{-2} = T^{2 - (-2)} = T^4, 1/M=M11 / M = M^{-1}, and 1/L3=L31 / L^3 = L^{-3}.

Key Concept

Dimensional analysis of physical constants in electromagnetism
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