Exams › JEE Main › Physics › Motion in a Plane
248 questions with worked solutions.
Answer: 10 m toward the west
North 30 -> (0,30); East 20 -> (20,30); 30sqrt2 SW = (-30,-30) -> (-10,0). Net displacement is 10 m due west.
Answer: (v)/(a)cosα
The correct option is derived from analyzing the relative velocity between the two particles. The minimum relative velocity occurs when the rate of change of the distance between them is zero, which can be mathematically expressed using the cosine of the angle between their paths, leading to the formula (v)/(a) ext{cos} alpha.
Answer: t = (π)/(ω)
A.B = cos(wt)cos(wt/2) + sin(wt)sin(wt/2) = cos(wt - wt/2) = cos(wt/2). Setting this to zero gives wt/2 = pi/2, hence t = pi/w.
Answer: 70.7 km/h toward the south-west
Initial velocity 50 km/h north, final 50 km/h (after 90 deg turn, e.g. west). Change = vf - vi = (west) + (-north), a vector of magnitude sqrt(50^2 + 50^2) = 70.7 km/h directed toward the south-west (not north-west, since we subtract the original northward velocity).
Answer: 150°
R=A+B perp to A: A^2 + A.B = 0. |R|^2 = A^2+2A.B+B^2 = B^2-A^2 = B^2/4 -> A^2 = 3B^2/4. cos(theta)=A.B/(AB) = -A^2/(AB) = -A/B = -sqrt3/2, so theta = 150 deg.
Answer: u î - (u)/(tanθ) ĵ
When the man moves at u and rain looks vertical, the rain's horizontal velocity equals u. At speed 2u the apparent horizontal component is u (backward), and tan(theta) = u/|v_y| gives |v_y| = u/tan(theta) downward. So the rain's ground velocity is u i - (u/tan(theta)) j.
Answer: 30°
Maximum height H = u^2 sin^2(theta)/(2g). Equal heights give uA^2 sin^2(45) = uB^2 sin^2(thetaB). With uB = sqrt(2) uA: uA^2 (1/2) = 2 uA^2 sin^2(thetaB) -> sin^2(thetaB) = 1/4 -> sin(thetaB) = 1/2 -> thetaB = 30 degrees.
Answer: π² m s⁻² and directed along the radius toward the centre
22 rev in 44 s gives T = 2 s, so w = 2*pi/T = pi rad/s. Centripetal acceleration = w^2 r = pi^2 * 1 = pi^2 m/s^2, directed along the radius toward the centre.
Answer: The velocity is perpendicular to r and the acceleration points toward the origin
r=(cos wt, sin wt). v=(-w sin wt, w cos wt) gives v.r=0, so velocity is perpendicular to r. a=(-w^2 cos wt, -w^2 sin wt)=-w^2 r, i.e. centripetal, pointing toward the origin (antiparallel to r), not perpendicular.
Answer: 5 h
Take A at origin moving west (-10,0) and B at (0,-100) moving north (0,10). Separation squared = (10t)^2 + (10t-100)^2; minimizing gives 200t + 200t - 2000 = 0, so t = 5 h.
Answer: tan⁻¹(1/2)
For launch angle 45 deg, range R = u^2/g and max height H = u^2/(4g) at horizontal distance R/2 = u^2/(2g). The elevation angle from launch point satisfies tan(theta) = H/(R/2) = (u^2/4g)/(u^2/2g) = 1/2, so theta = tan^-1(1/2).
Answer: The magnitude of the particle’s velocity is 8 m/s
R = 4 sin(2*pi*t) i + 4 cos(2*pi*t) j describes uniform circular motion of radius 4 m with omega = 2*pi rad/s, so speed v = omega*R = 8*pi ~ 25.1 m/s. The statement 'velocity is 8 m/s' is therefore the incorrect one; the centripetal results (a = v^2/R, directed along -R) are all correct.
Answer: 90°
Squaring |A+B|=|A-B| gives 4 A.B = 0, so A.B = 0 and the angle between A and B is 90 deg.
Answer: √(2(u² − gl))
The correct option is derived from the conservation of mechanical energy. At the lowest point, the stone has kinetic energy due to its speed u, and as it rises to the horizontal position, some of this energy is converted into potential energy, resulting in a change in velocity that can be expressed as √(2(u² - gl)).
Answer: M performs simple harmonic motion
The foot M tracks the x-coordinate of P, which equals a*cos(theta). Since dtheta/dt is constant, theta = w*t and x_M = a*cos(w*t), so M executes simple harmonic motion.
Answer: 9
On axis, E/B = x*c^2/(2*pi*f*R^2), so E/(cB) = x*c/(2*pi*f*R^2) = (0.2*3e8)/(2*pi*1e4*0.01) = 9.55e4. Then u_E/u_B = (E/(cB))^2 = 9.1e9, giving a = 9.
Answer: 7.421 MeV
Using B = 2*pi*m*f/q, KE = (B^2 q^2 r^2)/(2m) = 2*pi^2*m*r^2*f^2 = 2*pi^2*(1.67e-27)*(0.6)^2*(1e7)^2 = 1.19e-12 J = about 7.42 MeV.
Answer: (b) Statement 1 is true, Statement 2 is true, and Statement 2 correctly explains Statement 1.
Statement 1 is true because two stones with different velocities will follow different trajectories and cannot meet in mid-air. Statement 2 is also true as it describes that if two particles have zero relative acceleration, their distance will either remain constant or increase, which aligns with the idea that differing velocities prevent them from converging.
Answer: 8.66 m
The correct option is right because the horizontal distance traveled by the ball can be calculated using the horizontal component of the initial velocity and the time it takes to reach the height of 10 m. By applying the kinematic equations for projectile motion, we find that the ball lands 8.66 m away from the throwing point.
Answer: 3t²√(α² + β²)
The speed of the particle is derived from the derivatives of its position coordinates with respect to time. By differentiating x and y with respect to t, we find the velocity components, and using the Pythagorean theorem to combine them gives the speed as 3t²√(α² + β²).
Answer: R
The time of flight for a projectile is influenced by the range and the angle of projection. When two angles yield the same range, the product of their respective times of flight is directly proportional to the range itself, as derived from the equations of motion for projectile motion.
Answer: The acceleration vector is tangent to the circle
The statement is false because, for a particle moving in a circle at constant angular speed, the acceleration vector, known as centripetal acceleration, always points towards the center of the circle, not tangentially along the path.
Answer: Yes, 60°
The person can catch the ball if they run at the same speed as the ball's horizontal component of motion. At an angle of 60°, the vertical and horizontal components of the ball's trajectory allow the runner to reach the same horizontal distance as the ball when it lands, making it possible for the catch.
Answer: 7√2 units
The final velocity can be calculated by adding the initial velocity to the product of acceleration and time. After 10 seconds, the resultant velocity vector's magnitude is found to be 7√2 units, confirming that option A is correct.
Answer: y² = x² + constant
vx = dx/dt = k y and vy = dy/dt = k x, so dy/dx = x/y -> y dy = x dx -> y^2/2 = x^2/2 + C -> y^2 = x^2 + constant.
Answer: -(v²)/(R)cosθ î - (v²)/(R)sinθ ĵ
In uniform circular motion the acceleration is purely centripetal, directed from P(R,theta) toward the center, i.e. opposite the radial unit vector (cos theta i + sin theta j). Hence a = -(v^2/R)cos theta i - (v^2/R)sin theta j.
Answer: π (v⁴)/(g²)
Water reaches farthest at 45 deg, giving max range R = v^2/g. The wet region is a circle of that radius, so area = pi*R^2 = pi*v^4/g^2.
Answer: 20 m
Thrown straight up to H = 10 m means u^2/(2g) = 10, so u^2 = 20g. The maximum horizontal range (at 45 degrees) is R = u^2/g = 20 m.
Answer: y = 2x - 5x²
Here ux = 1, uy = 2, so tan(theta) = 2 and the trajectory is y = 2x - (g/(2 ux^2)) x^2 = 2x - (10/2) x^2 = 2x - 5x^2.
Answer: y² = x² + constant
The correct option describes a relationship between x and y that arises from the particle's velocity components, which are proportional to each other. By integrating the velocity components, we find that the path of the particle follows a quadratic relationship, specifically in the form of a circle or parabola, leading to the equation y² = x² + constant.
Answer: (c) πR⁴σω / 4
For a ring radius r: dq = sigma*2pi r dr, current di = dq*omega/2pi = sigma*omega*r dr, dm = di*pi r^2 = pi*sigma*omega*r^3 dr. Integrating 0 to R gives m = pi*sigma*omega*R^4/4.
Answer: u cos α / f
Relative speed squared = u^2 + (ft)^2 - 2u(ft)cos(alpha). Differentiating with respect to t and setting to zero: 2f^2 t - 2uf cos(alpha)=0, so t = u cos(alpha)/f.
Answer: 40 m
The height of the pole can be determined using the tangent of the angle subtended, which relates the height of the pole to the distance from the foot. Given that the angle is tan⁻¹(3/5), we can set up the relationship using the tangent function, leading to a height of 40 m for the upper 3/4 portion of the pole.
Answer: 20√2 m
The correct option is right because, using the kinematic equations, the position of the particle after 2 seconds can be calculated by adding the initial position to the displacement caused by the initial velocity and the acceleration. This results in a final position that, when calculated, gives a distance of 20√2 m from the origin.
Answer: √2 aω
vx=-a*w*sin(wt), vy=a*w*cos(wt), vz=a*w. Speed = sqrt(a^2 w^2 (sin^2+cos^2) + a^2 w^2) = sqrt(2) * a * w.
Answer: m y0 aω2 k
At t = 0, the particle's position is (x0, y0), and the torque is calculated using the formula τ = r × F, where r is the position vector and F is the force. The force acting on the particle is its mass times acceleration, which is derived from the second derivatives of the position equations, leading to the correct torque expression of m y0 aω² k.
Answer: 50
r=15t^2 i +(4-20t^2) j gives a = r'' = 30 i - 40 j (constant). |a| = sqrt(30^2+40^2) = sqrt(2500) = 50.
Answer: 2s and 18m
The particle's x-coordinate can be calculated using the equation of motion, which shows that with a constant acceleration of 10 m/s², it reaches 20 m in 2 seconds. The y-coordinate can then be determined using the initial velocity and acceleration, resulting in a position of 18 m at that same time.
Answer: v is perpendicular to r and a is directed towards the origin
The velocity vector v(t) is derived from the position vector r(t) and represents the tangent to the circular path, making it perpendicular to r. The acceleration vector a(t), which is centripetal in this case, points towards the center of the circular motion, thus directed towards the origin.
Answer: 60
From y = (1/2)(4)t^2 = 2t^2 = 32, t = 4 s. Then x = 3t + (1/2)(6)t^2 = 12 + 48 = 60 m.
Answer: 3√3 u² / 8g
At apex vx=u/2, vy=0, height H=u^2 sin^2(60)/(2g)=3u^2/(8g). Inelastic collision with mass m moving at u gives combined vx=(u/2+u)/2=3u/4. Fall time t=sqrt(2H/g)=u*sqrt(3)/(2g), so horizontal distance = (3u/4)*t = 3*sqrt(3)*u^2/(8g).
Answer: 39.55 m
The minimum height of the receiving antenna is determined by the line of sight distance, which depends on the curvature of the Earth. Using the formula for line of sight, the height required for a 45 km distance results in approximately 39.55 m, ensuring that the antenna can receive signals without obstruction.
Answer: 15
r x a = b x r means r x a = -(r x b), so r x (a+b) = 0 and r is parallel to a+b = (3,-1,2); write r = t(3,-1,2). The conditions r.(alpha,2,1)=3 and r.(2,5,-alpha)=-1 give t=1, alpha=1, so |r|^2 = 9+1+4 = 14 and alpha + |r|^2 = 15.
Answer: cos⁻¹((n²−1)/(n²+1))
The correct option is derived from the relationship between the magnitudes of the sum and difference of two vectors, which can be expressed in terms of the cosine of the angle between them. By applying the law of cosines and manipulating the resulting equations, we find that the angle can be expressed as cos⁻¹((n²−1)/(n²+1)), which matches the given condition.
Answer: 15m
The butterfly's velocity can be broken down into its north and east components, and when combined with the wind's southward velocity, the resultant velocity leads to a net displacement. Over 3 seconds, this results in a total displacement of 15 meters.
Q46. Choose the correct option:
Answer: True dip is less than apparent dip.
Apparent dip is measured in a vertical plane not containing the magnetic meridian: tan(delta') = tan(delta)/cos(theta) >= tan(delta). Hence the true dip is always less than (or equal to) the apparent dip.
Answer: Height = 1731 m Population Covered = 1413 × 10⁵
Coverage radius d = sqrt(2*Re*h) -> h = d^2/(2*Re) = (150000)^2/(2*6.5e6) = 1731 m. Population = 2000 * pi * d^2 = 2000 * pi * (150)^2 = 1413 x 10^5.
Answer: cos⁻¹((n²−1)/(−n²+1))
The correct option is derived from the relationship between the magnitudes of the vectors and the cosine of the angle between them. By applying the law of cosines to the expressions for the magnitudes of (X - Y) and (X + Y), we can establish a relationship that simplifies to the given expression for the angle.
Answer: straight line vertically down the plane
To the observer in the plane, the bomb has zero horizontal velocity relative to the plane, so it appears to drop vertically straight down.
Answer: T ∝ R²
The time period of revolution for a particle moving in a circular path is related to the radius and the centripetal force acting on it. Since the fictitious force is inversely proportional to R³, the centripetal acceleration is proportional to F/R, leading to a relationship where the time period T is proportional to R².