acceleration vector वाक्य
उदाहरण वाक्य
मोबाइल
- But your " acceleration vector " still points due east ( it is the same in all reference frames ), so viewed from the ground your acceleration is not perpendicular to your velocity.
- Most of the time, I imagine, " fire whenever the target acceleration vector is below your horizon " is enough control . talk ) 20 : 24, 24 February 2015 ( UTC)
- The acceleration vector of \ gamma is defined by \ nabla _ { \ dot \ gamma } { \ dot \ gamma }, where \ nabla denotes the covariant derivative associated to \ Gamma.
- Acceleration and force are vectors ( as indicated by their symbols being displayed in slant bold font ); in this law the direction of the force vector is the same as the direction of the acceleration vector.
- While the room orbits the earth, you and your friend actually experience slightly different gravitational acceleration vectors, and will ever so slowly move toward one another, though this may be too slight to be perceptible.
- The torque vector is perpendicular to the plane defined by the force and the vector \ scriptstyle \ vec r, and in this example it is directed towards the observer; the angular acceleration vector has the same direction.
- 1913 : von Laue used in the second edition of his book only Minkowski's acceleration vector ( for which he coined the name " four-acceleration ( ) ) instead of the transformation of three-acceleration.
- For the case of constant acceleration, the differential equation Eq 1 ) can be integrated as the acceleration vector "'A "'of a point " P " is constant in magnitude and direction.
- The angular velocity of the precession is a maximum if the velocity and acceleration vectors are perpendicular throughout the motion ( a circular orbit ), and is large if their magnitudes are large ( the magnitude of is almost ).
- Then the appearance of the night sky is transformed in exactly the manner described by the one-parameter subgroup of hyperbolic transformations sharing the fixed points 0, ", with the real number ? corresponding to the magnitude of his acceleration vector.
- Any point that is rigidly connected to the body can be used as reference point ( origin of coordinate system " L " ) to describe the linear motion of the body ( the linear position, velocity and acceleration vectors depend on the choice ).
- If the direction upward is taken as positive ( the normal cartesian convention ) then " positive " g-force ( an acceleration vector that points upward ) produces a force / weight on any mass, that acts " downward " ( an example is positive-g acceleration of a rocket launch, producing downward weight ).
- In the same way that we found the Lema�tre observers, we can boost our static frame in the \ vec { e } _ 3 direction by an undetermined parameter ( depending on the radial coordinate ), compute the acceleration vector, and require that this vanish " in the equatorial plane " \ theta = \ pi / 2.
- Where "'F "'is the vector sum of all forces exerted on the vehicle, m is its current mass, and "'a "'is the acceleration vector, the instantaneous rate of change of velocity ( "'v "'), which in turn is the instantaneous rate of change of displacement.
- Computing the kinematic decomposition of the timelike congruence defined by the timelike unit vector field \ scriptstyle \ vec { f } _ 0, we find that the expansion and vorticity again vanishes, and in addition the acceleration vector vanishes, \ scriptstyle \ nabla _ { \ vec { f } _ 0 } \ vec { f } _ 0 \; = \; 0.
- In the same way, a " negative-g force " is an acceleration vector " downward " ( the negative direction on the y axis ), and this acceleration downward produces a weight-force in a direction " upward " ( thus pulling a pilot upward out of the seat, and forcing blood toward the head of a normally oriented pilot ).
- Here \ boldsymbol { U } is the velocity field of the air, \ boldsymbol { \ Omega } is the angular velocity vector of the planet, \ rho is the density of the air, p is the air pressure, \ boldsymbol { F } _ r is the friction, \ boldsymbol { g } is the acceleration vector due to gravity and { D \; \ over Dt } is the material derivative.
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