This question is related to vertors and mechanical equilibrium
If:
angle theta 1=120 degrees
angle theta 2=210 degrees
angle theta 3= 0 degrees
mass 3= 500g
What are the values for the masses m1 and m2? Draw a proper vector diagram of this.
This question is related to vertors and mechanical equilibrium If: angle theta 1=120 degrees angle theta...
A block with mass m1=200 g is on a plane that makes an angle theta = 30 degrees above the horizontal. The coefficient of kinetic friction between m1 and the plane is "mu k"= 0.10. Mass m1 is attached by a string to another mass, m2 = 250g, which hangs freely as shown in the picture provided. Block m2 accelerates downward once it is set in motion. Assume pulleys is frictionles and the weight of the string is negligible. a)...
A block with mass m1=200 g is on a plane that makes an angle theta = 30 degrees above the horizontal. The coefficient of kinetic friction between m1 and the plane is "mu k"= 0.10. Mass m1 is attached by a string to another mass, m2 = 250g, which hangs freely as shown in the picture provided. Block m2 accelerates downward once it is set in motion. Assume pulleys is frictionles and the weight of the string is negligible. a)...
A block with mass m1=200 g is on a plane that makes an angle theta = 30 degrees above the horizontal. The coefficient of kinetic friction between m1 and the plane is "mu k"= 0.10. Mass m1 is attached by a string to another mass, m2 = 250g, which hangs freely as shown in the picture provided. Block m2 accelerates downward once it is set in motion. Assume pulleys is frictionles and the weight of the string is negligible. a)...
A block with mass m1=200 g is on a plane that makes an angle theta = 30 degrees above the horizontal. The coefficient of kinetic friction between m1 and the plane is "mu k"= 0.10. Mass m1 is attached by a string to another mass, m2 = 250g, which hangs freely as shown in the picture provided. Block m2 accelerates downward once it is set in motion. Assume pulleys is frictionles and the weight of the string is negligible. a)...
Consider the system of two masses connected by weightless strings on the right: A box of mass m1=1kg sits on an inclined, frictionless surface with an angle of a = 30 degrees. A second mass hangs from the ceiling with an angle of q = 30 degrees. A string parallel to the inclined surface connects both masses. The system is in equilibrium and does not move. 1) Draw a free body diagram of mass 1 and mass 2 and label...
A block of mass m is sliding down a plane inclined at an angle theta to the horizontal. If the coefficient of friction is µk . Find the acceleration of the block. Draw a vector diagram to solve this question.
Forces in equilibrium: 1) Given F1 = 1.47 N , where m1 = .150kg and (1) = 210 (degrees) Determine two more forces (magnitude and direction), which are at right angles to each other, but neither of them parallel to F(1), such that when they are applied, the system will be in equilibrium. 2) Given m1 = .140 kg at (1) = 80 (degrees), and m2 = .180 kg at (2) = 220 (degrees) Determine the masses required in order...
Figure 4 shows a two-mass translational mechanical system. The applied force falt) acts on mass mi. Displacements z1 and 22 are absolute positions of masses mi and m2, respectively, measured relative to fixed coordinates (the static equilibrium positions with fa(t) = 0). An oil film with viscous friction coefficient b separates masses mi and m2. Draw the free body diagram and derive the mathematical model of the vibration system using the diagram. falt) Oil film, friction coefficient b K m2...
Question 1 0/1 pts Aladder leans against a wall, an angle theta from the horizontal direction. (that is, theta =0 would mean horizontal). The ladder has mass M, and a person of mass m stands at the center of the ladder. What is the minimum necessary coefficient of static friction mu_s with the ground, such that the ladder will not slip out? sin(theta) / (2 cos(theta)) cos(theta)/(2 sin(theta)) Msin(theta)/(2(M+m) cos(theta)) Mcos(theta)/(2(M+m) sin(theta)) 0 1 1 nts
The equations of motion for a certain mechanical system with two degrees of freedom, can be written as a pair of coupled, second-order, differential equations: (M + m)x - 1/2 mL theta^2 sin(theta) + 1/2 mL theta cos(theta) + k(x - L_0) = 0 1/3 mL^2 theta + 1/2 mLx cos(theta) + 1/2 mgLsin(theta) = 0 We can rewrite them in matrix form, A*qdd - b, to be solved simultaneously: [M + m 1/2 mL cos theta 1/2 mL cos...