All of that is fascinating information. Thank you for sharing.
Let's take east and west to be positive and negative, respectively, and north and south to be positive and negative, respectively. Then in terms of vectors (using ijk notation), the car first moves 200 km west,
r = (-200 km) j
then 80 km southwest,
s = (-80/√2 km) i + (-80/√2 km) j
so that its total displacement is
r + s = (-80/√2 km) i + ((-200 - 80/√2) km) j
r + s ≈ (-56.6 km) i + (-256.6 km) j
This vector has magnitude
√((-56.6 km)² + (-256.6 km)²) ≈ 262.7 km
and direction θ such that
tan(θ) = (-256.6 km) / (-56.6 km) ==> θ ≈ -102.4º
relative to east, or about 12.4º west of south.
Answer:
Explanation:
To find Depth D of lake we must need to find the time taken to hit the water.So we use equation of simple motion as:
Δx=vit+(1/2)at²
As we have find the time taken now we need to find the final velocity vf from below equation as
So the depth of lake is given by:
first we need to find total time as
t=3.0-1.01 =1.99 s
The rate of change of angulardisplacement is defined as angular velocity. The angular velocity will be 22.41rad/s.
The rate of change of angular displacement is defined as angular velocity. Its unit is rad/sec.
ω = θ t
Where,
θ is the angle of rotation,
tis the time
ω is the angular velocity
The given data in the problem is;
u is the initialvelocity=0
α is the angularacceleration = 4.0 rad/s²
t is the time period=
n is the number of revolution = 10 rev
From Newton's second equation of motion in terms of angular velocity;
Hence the angular velocity will be 22.41 rad/s.
To learn more about angularvelocity refer to the link
Answer:
= 22.41rad/s
Explanation:
First, we know that:
a = 4 rad/s^2
S = 10 rev = 62.83 rad
Now we know that:
where is the final angular velocity, the initial angular velocity, a is the angular aceleration and S the radians.
Replacing, we get:
Finally, solving for :
= 22.41rad/s
Swinging a tennis racket against a ball is an example of a third class lever.
OT
OF
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Please select the best answer from the choices provided.
K
Swinging a tennis racket against a ball as a third class lever in physics.
A tennis racket swinging against a ball is indeed an example of a third class lever in physics. In a third class lever, the effort is situated between the fulcrum and the load. In this case, the effort is provided by the player's hand gripping the racket handle, the fulcrum is the wrist joint, and the load is the ball being struck by the racket.
When a player swings the racket, the force applied by the player's hand exerts an effort on the handle of the racket. This causes the racket to rotate about the wrist joint acting as the fulcrum. The ball serves as the load, receiving the force and accelerating in the opposite direction.