Thus, for a body to be at equilibrium, not only must the net force on it be equal to zero but the net torque with respect to any point must also be zero.
Some components inz ∈ (F Q )1 × ∣ E∣ can be equal to zero, and no components in z ∈ (F Q )1 × ∣ E∣ can be equal to zero.
For the above matrix to have non-trivial solution, its determinant must be equal to zero.
In all these cases we impose the log to be equal to zero.
The remaining unknown constant (i.e., E k ) will be obtained to be equal to zero.
For the ES coefficient, the null hypothesis is to be equal to zero.
In this case, the impact of automatic stabilizers on current demand would be equal to zero.
First, the displacement (w) must be equal to zero at the edges and any moment that coincides in direction with the direction of the edge must be equal to zero.
where is a constant, and are constants that may or may not be equal to zero, may be equal to zero or may be a polynomial in,, and are polynomials in with.
where and are polynomials in with, and are constants that may or may not be equal to zero.
In addition, based on equation 22 in [4], the achievable multiplexing gain should be equal to zero.
