Mechanics

227 soru

Soru 121Soru

A stone is thrown into the air with an initial velocity of 20 m/s20\text{ m/s} at an angle of 6060^\circ to the horizontal. What is the magnitude of its velocity at the highest point of its trajectory?

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Cevap: 10 m/s10\text{ m/s}

Cevap

The magnitude of the velocity at the highest point is 10 m/s10\text{ m/s}.
At the peak of a projectile's trajectory, the vertical velocity component vanishes (vy=0 m/sv_y = 0\text{ m/s}), but horizontal motion continues at a constant speed (vx=ucosθv_x = u \cos \theta). Substituting u=20 m/su = 20\text{ m/s} and θ=60\theta = 60^\circ yields vx=20×0.5=10 m/sv_x = 20 \times 0.5 = 10\text{ m/s}.

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1
Identify the velocity components at the apex
At maximum height, the vertical velocity component is vy=0 m/sv_y = 0\text{ m/s}, while the horizontal component remains constant at vx=ux=ucosθv_x = u_x = u \cos \theta.
Horizontal acceleration is zero when air resistance is neglected.
2
Calculate the horizontal component of velocity
vx=20×cos(60)=20×0.5=10 m/sv_x = 20 \times \cos(60^\circ) = 20 \times 0.5 = 10\text{ m/s}.
The trigonometric cosine function gives the horizontal projection of the initial velocity vector.
3
Determine total velocity magnitude at the apex
v=vx2+vy2=102+02=10 m/sv = \sqrt{v_x^2 + v_y^2} = \sqrt{10^2 + 0^2} = 10\text{ m/s}.
Since the vertical component is zero, the total velocity at the peak equals the horizontal component.

Anahtar Kavram

Velocity components at maximum height in projectile motion
Soru 122Soru

A body is projected from ground level with an initial speed of 40 m/s40\text{ m/s} at an angle of 3030^\circ to the horizontal. Calculate the time taken, in seconds, for the body to reach its maximum height. (Take g=10 m/s2g = 10\text{ m/s}^2)

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Cevap: 2

Cevap

The time taken to reach maximum height is 2 s2\text{ s}.
The initial vertical velocity component is uy=usin(30)=40×0.5=20 m/su_y = u \sin(30^\circ) = 40 \times 0.5 = 20\text{ m/s}. Under gravitational deceleration (g=10 m/s2g = 10\text{ m/s}^2), the vertical speed drops to zero at maximum height after t=uyg=2010=2 st = \frac{u_y}{g} = \frac{20}{10} = 2\text{ s}.

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1
Find the vertical component of initial velocity (uyu_y)
uy=40sin(30)=20 m/su_y = 40 \sin(30^\circ) = 20\text{ m/s}
Only the vertical component of initial velocity determines the time to reach maximum height.
2
Calculate the time to maximum height (tt)
t=uyg=2010=2 st = \frac{u_y}{g} = \frac{20}{10} = 2\text{ s}
At maximum height, vertical velocity vy=0v_y = 0, giving t=uygt = \frac{u_y}{g}.

Anahtar Kavram

Time to reach maximum height in projectile motion
Soru 123Soru

An autonomous drone navigating an obstacle course experiences three mutually perpendicular velocity vectors simultaneously: a horizontal forward velocity of 12 m s112\text{ m s}^{-1} due East, a horizontal crosswind drift velocity of 9 m s19\text{ m s}^{-1} due North, and a vertical downdraft velocity of 8 m s18\text{ m s}^{-1} directed straight downward. What is the magnitude of the resultant velocity vector of the drone in m s1\text{m s}^{-1}?

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Cevap: 17

Cevap

17 m s⁻¹
Because the three velocity components are mutually perpendicular, the magnitude of the overall resultant velocity is calculated using the 3D Pythagorean theorem: 122+92+82=144+81+64=289=17 m s1\sqrt{12^2 + 9^2 + 8^2} = \sqrt{144 + 81 + 64} = \sqrt{289} = 17\text{ m s}^{-1}.

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1
Identify the perpendicular vector components
vx=12 m s1v_x = 12\text{ m s}^{-1}, vy=9 m s1v_y = 9\text{ m s}^{-1}, vz=8 m s1v_z = 8\text{ m s}^{-1}
The three given velocity vectors act along mutually orthogonal spatial axes (East, North, and Downward).
2
Apply the 3D vector resultant magnitude formula
vr=vx2+vy2+vz2v_r = \sqrt{v_x^2 + v_y^2 + v_z^2}
Since the vector components are perpendicular to one another, the magnitude of their resultant is given by the extension of the Pythagorean theorem to three dimensions.
3
Substitute values and evaluate
vr=144+81+64=289=17 m s1v_r = \sqrt{144 + 81 + 64} = \sqrt{289} = 17\text{ m s}^{-1}
Squaring each component, adding them, and taking the principal square root yields the total magnitude of the velocity vector.

Anahtar Kavram

Magnitude of three mutually perpendicular vector components using the 3D Pythagorean theorem
Soru 124Soru

A cannonball is fired from level ground with an initial speed of 20 m/s20\text{ m/s} at an angle of 3030^\circ above the horizontal. Taking the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the total time of flight of the cannonball before it returns to ground level?

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Cevap: 2.0 s2.0\text{ s}

Cevap

2.0 s2.0\text{ s}
The correct answer of 2.0 s2.0\text{ s} is determined by resolving the initial speed into its vertical component uy=20sin30=10 m/su_y = 20 \sin 30^\circ = 10\text{ m/s} and using the total time of flight formula T=2usinθg=2(10)10=2.0 sT = \frac{2 u \sin \theta}{g} = \frac{2(10)}{10} = 2.0\text{ s}.

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1
Calculate the vertical component of the initial velocity (uyu_y).
uy=usinθ=20×sin30=20×0.5=10 m/su_y = u \sin \theta = 20 \times \sin 30^\circ = 20 \times 0.5 = 10\text{ m/s}
Only the vertical component of velocity determines the time the projectile remains in the air.
2
Calculate the total time of flight (TT) using the kinematic formula for full trajectory.
T=2uyg=2×1010=2.0 sT = \frac{2 u_y}{g} = \frac{2 \times 10}{10} = 2.0\text{ s}
The total time of flight includes both the time to ascend to peak height and descend back to the launch height under gravity gg.

Anahtar Kavram

Total Time of Flight in Projectile Motion
Soru 125Soru

A particle is projected from ground level at an angle to the horizontal. At its highest point of trajectory, which of the following statements correctly describes its velocity and acceleration?

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Cevap: The vertical component of velocity is zero, the horizontal component of velocity is non-zero, and the acceleration is directed downward.

Cevap

At the highest point of projectile motion, the vertical velocity component is zero, the horizontal velocity component is non-zero, and acceleration due to gravity acts downward.
At the peak of a projectile trajectory, vertical upward velocity is fully decelerated by gravity to zero. However, horizontal velocity is maintained because there is no horizontal acceleration. Acceleration due to gravity continues to act constantly downward.

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1
Analyze vertical velocity at the highest point
vy=0v_y = 0
At maximum height, the upward vertical component of motion reduces to zero before the particle begins descending.
2
Analyze horizontal velocity throughout motion
vx=ucosθ0v_x = u \cos\theta \neq 0
In the absence of air resistance, no horizontal force acts on the projectile, keeping horizontal velocity constant throughout flight.
3
Determine the direction of acceleration
a=ga = g acting vertically downward
Gravity is the only force acting on a projectile in motion, providing continuous downward acceleration.

Anahtar Kavram

Velocity components and acceleration at the apex of projectile motion
Tahmini Süre:45s
Soru 126Soru

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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Cevap: 15

Cevap

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}.

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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.

Anahtar Kavram

Multi-stage vertical motion under constant acceleration followed by free-fall under gravity
Soru 127Soru

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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Cevap: 2

Cevap

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.

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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.

Anahtar Kavram

Dimensional Analysis and Dimensional Homogeneity
Tahmini Süre:1m 30s
Soru 128Soru

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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Cevap: 1.0 m s1-1.0\text{ m s}^{-1}

Cevap

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.

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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.

Anahtar Kavram

Law of Conservation of Linear Momentum and Newton's Third Law of Motion
Tahmini Süre:45s
Soru 129Soru

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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Cevap: 50

Cevap

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}.

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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}.

Anahtar Kavram

Interdependence of Maximum Height, Range, and Launch Velocity in Projectile Motion
Tahmini Süre:1m 30s
Soru 130Soru

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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Cevap: 20 m20\text{ m}

Cevap

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}.

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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.

Anahtar Kavram

Kinematic Equation for Linear Distance Under Uniform Acceleration
Tahmini Süre:45s
Soru 131Soru

An object is projected from level ground with an initial speed of 30 m/s30\text{ m/s} at an angle of 3030^\circ to the horizontal. Taking the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, calculate the maximum height reached by the object in meters.

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Cevap: 11.25

Cevap

The maximum height reached by the object is 11.25 m11.25\text{ m}.
The vertical component of initial velocity is uy=30sin(30)=15 m/su_y = 30 \sin(30^\circ) = 15\text{ m/s}. At maximum height, vertical velocity becomes zero, so H=uy22g=15220=11.25 mH = \frac{u_y^2}{2g} = \frac{15^2}{20} = 11.25\text{ m}.

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1
Calculate the vertical component of the initial velocity.
uy=usinθ=30×sin(30)=15 m/su_y = u \sin\theta = 30 \times \sin(30^\circ) = 15\text{ m/s}
Only the vertical component of initial velocity determines the maximum height.
2
Apply the vertical motion equation at maximum height where vertical velocity is zero.
H=uy22g=1522×10=11.25 mH = \frac{u_y^2}{2g} = \frac{15^2}{2 \times 10} = 11.25\text{ m}
Using vy2=uy22gHv_y^2 = u_y^2 - 2gH with vy=0v_y = 0 gives H=uy22gH = \frac{u_y^2}{2g}.

Anahtar Kavram

Maximum height of a projectile
Tahmini Süre:45s
Soru 132Soru

The torque τ\tau required to rotate a thin flat disk of radius rr at a constant angular velocity ω\omega in a fluid of dynamic viscosity η\eta is expressed by the dimensional formula τ=kηxωyrz\tau = k \eta^x \omega^y r^z, where kk is a dimensionless constant. What is the value of the sum of the exponents x+y+zx + y + z?

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Cevap: 5

Cevap

The sum of the exponents x+y+zx + y + z is 5.
By substituting the base dimensions into τ=kηxωyrz\tau = k \eta^x \omega^y r^z, we get ML2T2=(ML1T1)x(T1)yLz=MxLx+zTxyM L^2 T^{-2} = (M L^{-1} T^{-1})^x (T^{-1})^y L^z = M^x L^{-x+z} T^{-x-y}. Equating exponents of MM gives x=1x = 1. Equating exponents of TT gives 1y=2    y=1-1 - y = -2 \implies y = 1. Equating exponents of LL gives 1+z=2    z=3-1 + z = 2 \implies z = 3. Thus, x+y+z=1+1+3=5x + y + z = 1 + 1 + 3 = 5.

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1
Determine the dimensions of torque, dynamic viscosity, angular velocity, and radius in base mechanical dimensions (M, L, T).
[τ]=ML2T2[\tau] = M L^2 T^{-2}, [η]=ML1T1[\eta] = M L^{-1} T^{-1}, [ω]=T1[\omega] = T^{-1}, and [r]=L[r] = L.
Dimensional analysis requires converting all parameters into base dimensions.
2
Apply the principle of dimensional homogeneity to set up exponential equations for each base dimension.
M1L2T2=MxLx+zTxyM^1 L^2 T^{-2} = M^x L^{-x+z} T^{-x-y}.
Both sides of a physically valid equation must share identical net dimensions.
3
Solve for each exponent individually by comparing indices.
x=1x = 1, y=1y = 1, z=3z = 3.
Matching powers of M yields x=1x=1, matching powers of T yields y=1y=1, and matching powers of L yields z=3z=3.
4
Sum the three calculated exponent values.
1+1+3=51 + 1 + 3 = 5.
The question asks specifically for the value of x+y+zx + y + z.

Anahtar Kavram

Dimensional analysis and dimensional homogeneity
Tahmini Süre:1m 30s
Soru 133Soru

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

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Cevap: 20

Cevap

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

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

Anahtar Kavram

Maximum height of a projectile depends entirely on its initial vertical component of velocity and acceleration due to gravity.
Soru 134Soru

What is the length of a simple pendulum that has a period of oscillation of 2.0 s2.0\text{ s} at a location where the acceleration due to gravity is g=π2 m/s2g = \pi^2\text{ m/s}^2?

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Cevap: 1.0 m1.0\text{ m}

Cevap

The length of the simple pendulum is 1.0 m1.0\text{ m}.
Using the period equation T=2πl/gT = 2\pi \sqrt{l/g}, squaring both sides yields T2=4π2l/gT^2 = 4\pi^2 l / g. Rearranging gives l=T2g4π2l = \frac{T^2 g}{4\pi^2}. Substituting T=2.0 sT = 2.0\text{ s} and g=π2 m/s2g = \pi^2\text{ m/s}^2 yields l=4π24π2=1.0 ml = \frac{4 \pi^2}{4 \pi^2} = 1.0\text{ m}.

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1
State the formula for the period of a simple pendulum.
T=2πlgT = 2\pi \sqrt{\frac{l}{g}}
This formula relates the oscillation period TT, pendulum length ll, and gravitational acceleration gg.
2
Square both sides of the equation to solve for ll.
T2=4π2(lg)    l=T2g4π2T^2 = 4\pi^2 \left(\frac{l}{g}\right) \implies l = \frac{T^2 \cdot g}{4\pi^2}
Isolating ll allows direct evaluation using the given numerical values.
3
Substitute T=2.0 sT = 2.0\text{ s} and g=π2 m/s2g = \pi^2\text{ m/s}^2 into the expression.
l=(2.0)2π24π2=4π24π2=1.0 ml = \frac{(2.0)^2 \cdot \pi^2}{4\pi^2} = \frac{4\pi^2}{4\pi^2} = 1.0\text{ m}
Simplifying by canceling π2\pi^2 and 44 gives the exact length.

Anahtar Kavram

Simple Pendulum Period and Length Relationship
Soru 135Soru

If a constant magnitude net force continuously acts on a moving body strictly perpendicular to its direction of motion, the magnitude of the body's linear momentum remains constant while its direction of motion continuously changes.

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Cevap: True

Cevap

The statement is True. A net force directed perpendicular to velocity changes only the direction of motion, keeping speed and the magnitude of linear momentum constant.
The statement is true because a force perpendicular to displacement does zero work, preserving kinetic energy and speed. Because speed is unchanged, the scalar magnitude of momentum remains constant while its vector direction curves continuously.

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1
Determine the work done by a perpendicular force.
The work done is W=FΔscos(90)=0 JW = F \Delta s \cos(90^\circ) = 0\text{ J}.
Force perpendicular to displacement performs no work on the object.
2
Relate work done to speed and magnitude of linear momentum.
Zero work means zero change in kinetic energy, so speed vv is constant, making magnitude p=mvp = mv constant.
Linear momentum magnitude depends solely on mass and speed.
3
Evaluate the effect on momentum direction.
The force produces an acceleration vector perpendicular to velocity, changing the vector direction of linear momentum p\vec{p}.
By Newton's Second Law (F=dpdt\vec{F} = \frac{d\vec{p}}{dt}), force dictates the rate of change of momentum vector.

Anahtar Kavram

Vector nature of linear momentum and perpendicular force action
Soru 136Soru

A cart of mass 40 kg40\text{ kg} carrying a package of mass 10 kg10\text{ kg} is coasting along a straight horizontal track at a constant velocity of 6.0 m s16.0\text{ m s}^{-1}. The package is suddenly ejected horizontally backward (opposite to the direction of motion of the cart) at a speed of 15 m s115\text{ m s}^{-1} relative to the ground. What is the new velocity of the cart after the package is ejected?

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Cevap: 11.25 m s111.25\text{ m s}^{-1}

Cevap

The new velocity of the cart is 11.25 m s111.25\text{ m s}^{-1} in the forward direction.
By the law of conservation of linear momentum, the total initial momentum of the system (cart plus package, 50 kg50\text{ kg} moving at 6.0 m s16.0\text{ m s}^{-1}) equals 300 kg m s1300\text{ kg m s}^{-1}. When the 10 kg10\text{ kg} package is ejected backward at 15 m s1-15\text{ m s}^{-1}, its momentum is 150 kg m s1-150\text{ kg m s}^{-1}. Setting 300=150+40vcart300 = -150 + 40 v_{\text{cart}} yields vcart=11.25 m s1v_{\text{cart}} = 11.25\text{ m s}^{-1}.

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1
Calculate the total initial momentum of the system before ejection.
Total mass mtotal=40 kg+10 kg=50 kgm_{\text{total}} = 40\text{ kg} + 10\text{ kg} = 50\text{ kg}. Initial momentum Pi=50 kg×6.0 m s1=300 kg m s1P_i = 50\text{ kg} \times 6.0\text{ m s}^{-1} = 300\text{ kg m s}^{-1}.
The initial system consists of both the cart and the package moving together at 6.0 m s16.0\text{ m s}^{-1}.
2
Set up the expression for final momentum considering direction.
Taking the forward direction as positive, the package's velocity is vpkg=15 m s1v_{\text{pkg}} = -15\text{ m s}^{-1}. Final momentum Pf=(10×15)+(40×vcart)=150+40vcartP_f = (10 \times -15) + (40 \times v_{\text{cart}}) = -150 + 40 v_{\text{cart}}.
Linear momentum is a vector quantity, so opposite motion must be assigned a negative sign.
3
Apply the law of conservation of linear momentum (Pi=PfP_i = P_f) to solve for the cart's final velocity.
300=150+40vcart    450=40vcart    vcart=11.25 m s1300 = -150 + 40 v_{\text{cart}} \implies 450 = 40 v_{\text{cart}} \implies v_{\text{cart}} = 11.25\text{ m s}^{-1}.
In the absence of external forces on the system, total linear momentum is conserved.

Anahtar Kavram

Conservation of Linear Momentum
Tahmini Süre:2m 0s
Soru 137Soru

A stone is projected horizontally with a speed of 15 m/s15\text{ m/s} from the top of a vertical cliff of height 20 m20\text{ m}. Taking acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2, what is the magnitude of the velocity of the stone just before it strikes the ground?

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Cevap: 25 m/s25\text{ m/s}

Cevap

The magnitude of the velocity of the stone just before hitting the ground is 25 m/s25\text{ m/s}.
For a horizontally launched projectile, the horizontal velocity component remains constant at vx=15 m/sv_x = 15\text{ m/s}. The vertical component just before impact is found using vy2=uy2+2gh=0+2(10)(20)=400v_y^2 = u_y^2 + 2gh = 0 + 2(10)(20) = 400, giving vy=20 m/sv_y = 20\text{ m/s}. Combining these perpendicular components yields a total speed of v=152+202=25 m/sv = \sqrt{15^2 + 20^2} = 25\text{ m/s}.

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1
Identify horizontal velocity component
vx=15 m/sv_x = 15\text{ m/s}
Air resistance is neglected, so horizontal velocity remains constant throughout flight.
2
Calculate vertical velocity component just before impact using third equation of motion
vy2=uy2+2gh=02+2(10)(20)=400    vy=20 m/sv_y^2 = u_y^2 + 2gh = 0^2 + 2(10)(20) = 400 \implies v_y = 20\text{ m/s}
Initial vertical velocity uy=0 m/su_y = 0\text{ m/s} for horizontal projection; stone falls through a vertical displacement of 20 m20\text{ m} under gravity.
3
Compute total resultant velocity magnitude using Pythagorean theorem
v=vx2+vy2=152+202=225+400=625=25 m/sv = \sqrt{v_x^2 + v_y^2} = \sqrt{15^2 + 20^2} = \sqrt{225 + 400} = \sqrt{625} = 25\text{ m/s}
Horizontal and vertical velocity components are mutually perpendicular.

Anahtar Kavram

Horizontal Projection and Resultant Velocity Vector Synthesis
Tahmini Süre:2m 0s
Soru 138Soru

A wooden block of mass 4.0 kg4.0\text{ kg} is suspended vertically at rest. A bullet of mass 0.05 kg0.05\text{ kg} travelling horizontally at 400 m s1400\text{ m s}^{-1} strikes the block, passes completely through it, and emerges on the opposite side with a reduced speed of 100 m s1100\text{ m s}^{-1}. If a constant retarding force brings the moving block to rest in 0.25 s0.25\text{ s} after the bullet emerges, calculate the magnitude of this retarding force in newtons.

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Cevap: 60

Cevap

The magnitude of the retarding force acting on the block is 60 N60\text{ N}.
During the impact, the bullet loses momentum equal to Δp=0.05 kg×(400 m s1100 m s1)=15 N s\Delta p = 0.05\text{ kg} \times (400\text{ m s}^{-1} - 100\text{ m s}^{-1}) = 15\text{ N s}. By the conservation of linear momentum, this exact amount of momentum is gained by the block. Applying Newton's second law (F=ΔpΔtF = \frac{\Delta p}{\Delta t}), the magnitude of the constant retarding force needed to reduce the block's momentum to zero in 0.25 s0.25\text{ s} is F=15 N s0.25 s=60 NF = \frac{15\text{ N s}}{0.25\text{ s}} = 60\text{ N}.

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1
Calculate the momentum lost by the bullet during penetration.
Δpbullet=0.05 kg×(400 m s1100 m s1)=15 N s\Delta p_{\text{bullet}} = 0.05\text{ kg} \times (400\text{ m s}^{-1} - 100\text{ m s}^{-1}) = 15\text{ N s}
The momentum lost by the bullet equals its mass multiplied by the change in its horizontal velocity vector.
2
Determine the initial momentum imparted to the wooden block using the law of conservation of linear momentum.
pblock=Δpbullet=15 N sp_{\text{block}} = \Delta p_{\text{bullet}} = 15\text{ N s}
Since no external horizontal force acts during the collision impact, the momentum lost by the bullet is fully transferred to the block.
3
Calculate the retarding force required to bring the block to rest using the impulse-momentum theorem.
F=ΔpblockΔt=15 N s0.25 s=60 NF = \frac{\Delta p_{\text{block}}}{\Delta t} = \frac{15\text{ N s}}{0.25\text{ s}} = 60\text{ N}
According to Newton's second law of motion, the net force acting on a body equals the rate of change of momentum.

Anahtar Kavram

Conservation of Linear Momentum and Newton's Second Law
Soru 139Soru

For an object of constant mass moving at constant speed along a complete circular path, the net vector impulse imparted to the object over one full revolution is zero, even though a continuous centripetal force acts on the object throughout the motion.

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Cevap: True

Cevap

The statement is true because the impulse-momentum theorem states that net impulse equals the change in momentum (J=Δp\vec{J} = \Delta \vec{p}). After one full revolution, the object's initial and final velocity vectors are identical, resulting in zero change in momentum.
The statement is correct because linear momentum is a vector quantity. Over a complete circular revolution, the initial and final velocity vectors are identical in both magnitude and direction, making the change in momentum—and therefore the net vector impulse—equal to zero.

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1
Recall the vector definition of impulse and the impulse-momentum theorem.
The net impulse J\vec{J} acting on a body equals its change in linear momentum: J=Δp=pfpi=mvfmvi\vec{J} = \Delta \vec{p} = \vec{p}_f - \vec{p}_i = m\vec{v}_f - m\vec{v}_i.
Impulse is a vector quantity dependent on the initial and final states of momentum over the time interval.
2
Evaluate the velocity vector of the object after one complete circular revolution at constant speed.
Since the speed is constant and the trajectory completes a closed loop, the final velocity vector vf\vec{v}_f has the exact same magnitude and direction as the initial velocity vector vi\vec{v}_i.
A complete revolution returns the object to its starting point with its velocity pointing in the initial direction.
3
Calculate the change in momentum Δp\Delta \vec{p}.
Δp=m(vfvi)=m(0)=0\Delta \vec{p} = m(\vec{v}_f - \vec{v}_i) = m(0) = \vec{0}. Thus, net impulse J=0\vec{J} = \vec{0}.
Subtracting identical vectors yields zero vector magnitude.

Anahtar Kavram

Impulse-Momentum Theorem and Vector Nature of Linear Momentum
Tahmini Süre:1m 30s
Soru 140Soru

An electric crane lifts a load of 250 kg250\text{ kg} vertically upwards through a height of 12 m12\text{ m} in 10 s10\text{ s} at a constant speed. Taking the acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}, what is the useful output power of the crane in watts?

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Cevap: 3000

Cevap

The useful output power of the crane is 3000 W3000\text{ W}.
The work done in lifting the load vertically is equal to the gravitational potential energy gained, W=mgh=250×10×12=30,000 JW = mgh = 250 \times 10 \times 12 = 30,000\text{ J}. Power is the rate of doing work, so P=Wt=30,00010=3000 WP = \frac{W}{t} = \frac{30,000}{10} = 3000\text{ W}.

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1
Identify the given values
Mass m=250 kgm = 250\text{ kg}, height h=12 mh = 12\text{ m}, time t=10 st = 10\text{ s}, acceleration due to gravity g=10 m s2g = 10\text{ m s}^{-2}.
Extract values needed for work and power calculations.
2
Calculate the work done in lifting the load
W=mgh=250 kg×10 m s2×12 m=30,000 JW = mgh = 250 \text{ kg} \times 10 \text{ m s}^{-2} \times 12 \text{ m} = 30,000\text{ J}.
The work done against gravity equals the gain in gravitational potential energy.
3
Calculate the power output
P=Wt=30,000 J10 s=3000 WP = \frac{W}{t} = \frac{30,000\text{ J}}{10\text{ s}} = 3000\text{ W}.
Power is defined as the rate at which work is done (P=WtP = \frac{W}{t}).

Anahtar Kavram

Power as the rate of doing work against gravity
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