A car moving with a speed of 12 m/s is subjected to brakes which produces a deceleration of 6 m/s². The car takes 2 s to stop after the application of brakes. What is the distance covered by the car after the application of brakes?
- (a)12 m
- (b)24 m
- (c)36 m
- (d)48 m
Correct — A, 12 m. Take the initial speed as u = 12 m/s, the acceleration as a = −6 m/s² because the car is slowing, and the time as t = 2 s. Check first that the numbers are consistent: v = u + at gives 12 − 6 × 2 = 0, so the car does indeed come to rest exactly at the end of the two seconds, as the stem says. Now use s = ut + ½at², which gives 12 × 2 + ½ × (−6) × 4 = 24 − 12 = 12 m. Two independent routes confirm it. The relation v² = u² + 2as with v = 0 gives 0 = 144 − 12s, so s = 12 m. And since the deceleration is uniform, the average speed over the stop is simply the mean of the initial and final speeds, (12 + 0)/2 = 6 m/s, which over 2 s covers 12 m. The trap is planted in the second option: 24 m is what you get by multiplying the initial speed by the time and forgetting that the car is slowing down the whole way. A braking car covers exactly half the distance a car holding its speed would.
- (b)24 m — The distance the car would cover if it kept moving at 12 m/s for the full two seconds. It ignores the braking altogether, and it is exactly twice the right answer because uniform deceleration to rest halves the distance.
- (c)36 m — Neither the braked nor the unbraked distance. It comes out of mixing the numbers — for instance adding a spurious term rather than subtracting the ½at² correction.
- (d)48 m — Four times the correct value. It would follow from doubling the time or from adding 24 and 24, and it is far beyond what a car losing all its speed in two seconds can travel.
For motion in a straight line with uniform acceleration the three equations of motion apply: v = u + at, s = ut + ½at², and v² = u² + 2as. Deceleration is simply negative acceleration and is handled by giving a a negative sign rather than by changing the equations. On a velocity-time graph the motion here is a straight line falling from 12 m/s to zero over 2 s, and the distance travelled is the area under that line — a triangle of base 2 and height 12, which is 12 m.
The safest habit in a braking numerical is to check the given data for consistency before using it. Here u/|a| = 12/6 = 2 s, which matches the stated stopping time, so the numbers hang together and any answer above 24 m can be discarded at once. The graphical route is the fastest of all: draw the velocity-time line and take the area, which for a triangle is half base times height. It is also worth carrying the physical consequence, because the same relation governs road safety. The braking distance goes as the square of the speed through v² = u² + 2as, so doubling a vehicle's speed quadruples the distance it needs to stop.
- The three equations of uniformly accelerated motion are v = u + at, s = ut + ½at² and v² = u² + 2as.
- Deceleration is negative acceleration; here a = −6 m/s² with u = 12 m/s.
- The stopping time follows from v = u + at with v = 0, giving t = u divided by the magnitude of the deceleration, that is 2 s.
- Under uniform acceleration the average velocity is the mean of the initial and final velocities, here 6 m/s.
- The area under a velocity-time graph gives the displacement, and for this motion the graph is a triangle of area 12 m.
The 24 m option is the same problem with the braking left out.
- Using the initial speed for the whole interval, which produces the doubled answer.
- Entering the deceleration as positive and getting a distance larger than the unbraked one.
- Skipping the consistency check between the given deceleration and the given stopping time.
As a braking-distance numerical, as a find-the-stopping-time item, or as a graphical item on the area under a velocity-time curve.
A car is running on a road at a uniform speed of 60 km/hr. The net resultant force on the car is
- (a) Driving force in the direction of car’s motion
- (b) Resistance force opposite to the direction of car’s motion
- (c) An inclined force
- (d) Equal to zero
Answer(d) Equal to zero
The same car, with the acceleration set to zero instead. No acceleration means no net force; the moment the brakes are applied a net force appears and the equations of motion take over.
The speed of a car travelling on a straight road is listed below at successive intervals of 1 s : Time (s) 0 1 2 3 4 Speed (m/s) 0 2 4 6 8 Which of the following is/are correct ? The car travels 1. with a uniform acceleration of 2 m/s². 2. 16 m in 4 s. 3. with an average speed of 4 m/s. Select the correct answer using the code given below :
- (a) 1, 2 and 3
- (b) 2 and 3 only
- (c) 1 and 2 only
- (d) 1 only
Answer(a) 1, 2 and 3
The accelerating mirror image of this braking problem, worked from a table. Distance from the area under the line and average speed as the mean of the end values are the same two shortcuts that settle the CDS numerical.
CDS_GK_2021_II_Q222021A bus starting from a bus-stand and moving with uniform acceleration attains a speed of 20 km/h in 10 minutes. What is its acceleration?
- (a) 200 km/h²
- (b) 120 km/h²
- (c) 100 km/h²
- (d) 240 km/h²
Answer(b) 120 km/h²
The same first equation used in the opposite direction, and a reminder to keep units consistent. Ten minutes is one-sixth of an hour, so 20 divided by one-sixth gives 120 km per hour squared.
- practice — not a real PYQ
A body moving at 20 m/s is brought to rest by a uniform deceleration of 5 m/s². The distance it covers before stopping is
- (a)20 m
- (b)40 m
- (c)80 m
- (d)100 m
Answer(b) 40 m — from v² = u² + 2as with v = 0, 0 = 400 − 10s, so s = 40 m; the stop takes 4 s.
- practice — not a real PYQ
If the speed of a vehicle is doubled while the braking deceleration stays the same, its stopping distance becomes
- (a)the same
- (b)twice as long
- (c)three times as long
- (d)four times as long
Answer(d) four times as long — stopping distance follows u² divided by twice the deceleration, so it grows with the square of the speed.